Optical image capturing system

ABSTRACT

An optical image capturing system includes, along the optical axis in order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. At least one lens among the first to the sixth lenses has positive refractive force. The seventh lens can have negative refractive force, and both surfaces thereof are aspheric. At least a surface of the seventh lens has an inflection point. The lenses in the optical image capturing system which have refractive power include the first to the seventh lenses. The optical image capturing system can increase aperture value and improve the imaging quality for use in compact cameras.

BACKGROUND OF THE INVENTION 1. Technical Field

The present invention relates generally to an optical system, and moreparticularly to a compact optical image capturing system for anelectronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of the ordinaryphotographing camera is commonly selected from charge coupled device(CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor).In addition, as advanced semiconductor manufacturing technology enablesthe minimization of the pixel size of the image sensing device, thedevelopment of the optical image capturing system towards the field ofhigh pixels. Therefore, the requirement for high imaging quality israpidly raised.

The conventional optical system of the portable electronic deviceusually has five or six lenses. However, the optical system is asked totake pictures in a dark environment, in other words, the optical systemis asked to have a large aperture. The conventional optical system couldnot provide a high optical performance as required.

It is an important issue to increase the amount of light entering thelens. In addition, the modern lens is also asked to have severalcharacters, including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces ofseven-piece optical lenses (the convex or concave surface in thedisclosure denotes the geometrical shape of an image-side surface or anobject-side surface of each lens on an optical axis) to increase theamount of incoming light of the optical image capturing system, and toimprove imaging quality for image formation, so as to be applied tominimized electronic products.

In addition, when it comes to certain application of optical imaging,there will be a need to capture image via light sources with wavelengthsin both visible and infrared ranges, an example of this kind ofapplication is IP video surveillance camera, which is equipped with theDay & Night function. The visible spectrum for human vision haswavelengths ranging from 400 to 700 nm, but the image formed on thecamera sensor includes infrared light, which is invisible to human eyes.Therefore, under certain circumstances, an IR cut filter removable (ICR)is placed before the sensor of the IP video surveillance camera, inorder to ensure that only the light that is visible to human eyes ispicked up by the sensor eventually, so as to enhance the “fidelity” ofthe image. The ICR of the IP video surveillance camera can completelyfilter out the infrared light under daytime mode to avoid color cast;whereas under night mode, it allows infrared light to pass through thelens to enhance the image brightness. Nevertheless, the elements of theICR occupy a significant amount of space and are expensive, which impedeto the design and manufacture of miniaturized surveillance cameras inthe future.

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which utilizethe combination of refractive powers, convex surfaces and concavesurfaces of four lenses, as well as the selection of materials thereof,to reduce the difference between the imaging focal length of visiblelight and imaging focal length of infrared light, in order to achievethe near “confocal” effect without the use of ICR elements.

The term and its definition to the lens parameter in the embodiment ofthe present are shown as below for further reference.

The lens parameters related to the magnification of the optical imagecapturing system

The optical image capturing system can be designed and applied tobiometrics, for example, facial recognition. When the embodiment of thepresent disclosure is configured to capture image for facialrecognition, the infrared light can be adopted as the operationwavelength. For a face of about 15 centimeters (cm) wide at a distanceof 25-30 cm, at least 30 horizontal pixels can be formed in thehorizontal direction of an image sensor (pixel size of 1.4 micrometers(μm)). The linear magnification of the infrared light on the image planeis LM, and it meets the following conditions: LM≥0.0003, where LM=(30horizontal pixels)*(1.4 μm pixel size)/(15 cm, width of the photographedobject). Alternatively, the visible light can also be adopted as theoperation wavelength for image recognition. When the visible light isadopted, for a face of about 15 cm wide at a distance of 25-30 cm, atleast 50 horizontal pixels can be formed in the horizontal direction ofan image sensor (pixel size of 1.4 micrometers (μm)).

The lens parameter related to a length or a height in the lens:

For visible spectrum, the present invention may adopt the wavelength of555 nm as the primary reference wavelength and the basis for themeasurement of focus shift; for infrared spectrum (700-1000 nm), thepresent invention may adopt the wavelength of 850 nm as the primaryreference wavelength and the basis for the measurement of focus shift.

The optical image capturing system includes a first image plane and asecond image plane. The first image plane is an image plane specificallyfor the visible light, and the first image plane is perpendicular to theoptical axis; the through-focus modulation transfer rate (value of MTF)at the first spatial frequency has a maximum value at the central fieldof view of the first image plane; the second image plane is an imageplane specifically for the infrared light, and second image plane isperpendicular to the optical axis; the through-focus modulation transferrate (value of MTF) at the first spatial frequency has a maximum valuein the central of field of view of the second image plane. The opticalimage capturing system also includes a first average image plane and asecond average image plane. The first average image plane is an imageplane specifically for the visible light, and the first average imageplane is perpendicular to the optical axis. The first average imageplane is installed at the average position of the defocusing positions,where the values of MTF of the visible light at the central field ofview, 0.3 field of view, and the 0.7 field of view are at theirrespective maximum at the first spatial frequency. The second averageimage plane is an image plane specifically for the infrared light, andthe second average image plane is perpendicular to the optical axis. Thesecond average image plane is installed at the average position of thedefocusing positions, where the values of MTF of the infrared light atthe central field of view, 0.3 field of view, and the 0.7 field of vieware at their respective maximum at the first spatial frequency.

The aforementioned first spatial frequency is set to be half of thespatial frequency (half frequency) of the image sensor (sensor) used inthe present invention. For example, for an image sensor having the pixelsize of 1.12 μm or less, the quarter spatial frequency, half spatialfrequency (half frequency) and full spatial frequency (full frequency)in the characteristic diagram of modulation transfer function are atleast 110 cycles/mm, 220 cycles/mm and 440 cycles/mm, respectively.Lights of any field of view can be further divided into sagittal ray andtangential ray.

The focus shifts where the through-focus MTF values of the visiblesagittal ray at the central field of view, 0.3 field of view, and 0.7field of view of the optical image capturing system are at theirrespective maxima, are denoted by VSFS0, VSFS3, and VSFS7 (unit ofmeasurement: mm), respectively. The maximum values of the through-focusMTF of the visible sagittal ray at the central field of view, 0.3 fieldof view, and 0.7 field of view are denoted by VSMTF0, VSMTF3, andVSMTF7, respectively. The focus shifts where the through-focus MTFvalues of the visible tangential ray at the central field of view, 0.3field of view, and 0.7 field of view of the optical image capturingsystem are at their respective maxima, are denoted by VTFS0, VTFS3, andVTFS7 (unit of measurement: mm), respectively. The maximum values of thethrough-focus MTF of the visible tangential ray at the central field ofview, 0.3 field of view, and 0.7 field of view are denoted by VTMTF0,VTMTF3, and VTMTF7, respectively. The average focus shift (position) ofboth the aforementioned focus shifts of the visible sagittal ray atthree fields of view and focus shifts of the visible tangential ray atthree fields of view is denoted by AVFS (unit of measurement: mm), whichequals to the absolute value |(VSFS0+VSFS3+VSFS7+VTFS0+VTFS3+VTFS7)/6|.

The focus shifts where the through-focus MTF values of the infraredsagittal ray at the central field of view, 0.3 field of view, and 0.7field of view of the optical image capturing system are at theirrespective maxima, are denoted by ISFS0, ISFS3, and ISFS7 (unit ofmeasurement: mm), respectively. The average focus shift (position) ofthe aforementioned focus shifts of the infrared sagittal ray at threefields of view is denoted by AISFS (unit of measurement: mm). Themaximum values of the through-focus MTF of the infrared sagittal ray atthe central field of view, 0.3 field of view, and 0.7 field of view aredenoted by ISMTF0, ISMTF3, and ISMTF7, respectively. The focus shiftswhere the through-focus MTF values of the infrared tangential ray at thecentral field of view, 0.3 field of view, and 0.7 field of view of theoptical image capturing system are at their respective maxima, aredenoted by ITFS0, ITFS3, and ITFS7 (unit of measurement: mm),respectively. The average focus shift (position) of the aforementionedfocus shifts of the infrared tangential ray at three fields of view isdenoted by AITFS (unit of measurement: mm). The maximum values of thethrough-focus MTF of the infrared tangential ray at the central field ofview, 0.3 field of view, and 0.7 field of view are denoted by ITMTF0,ITMTF3, and ITMTF7, respectively. The average focus shift (position) ofboth of the aforementioned focus shifts of the infrared sagittal ray atthe three fields of view and focus shifts of the infrared tangential rayat the three fields of view is denoted by AIFS (unit of measurement:mm), which equals to the absolute value of|(ISFS0+ISFS3+ISFS7+ITFS0+ITFS3+ITFS7)/6|.

The focus shift (difference) between the focal points of the visiblelight and the infrared light at their central fields of view (RGB/IR) ofthe entire optical image capturing system (i.e. wavelength of 850 nmversus wavelength of 555 nm, unit of measurement: mm) is denoted by FS,which satisfies the absolute value |(VSFS0+VTFS0)/2−(ISFS0+ITFS0)/2|.The difference (focus shift) between the average focus shift of thevisible light in the three fields of view and the average focus shift ofthe infrared light in the three fields of view (RGB/IR) of the entireoptical image capturing system is denoted by AFS (i.e. wavelength of 850nm versus wavelength of 555 nm, unit of measurement: mm), which equalsto the absolute value of |AIFS−AVFS|.

A maximum height for image formation of the optical image capturingsystem is denoted by HOI. A height of the optical image capturing systemis denoted by HOS. A distance from the object-side surface of the firstlens to the image-side surface of the seventh lens is denoted by InTL. Adistance from the first lens to the second lens is denoted by IN12(instance). A central thickness of the first lens of the optical imagecapturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing systemis denoted by NA1 (instance). A refractive index of the first lens isdenoted by Nd1 (instance).

The lens parameter related to a view angle in the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. For any surface of any lens, a maximum effective halfdiameter (EHD) is a perpendicular distance between an optical axis and acrossing point on the surface where the incident light with a maximumviewing angle of the system passing the very edge of the entrance pupil.For example, the maximum effective half diameter of the object-sidesurface of the first lens is denoted by EHD11, the maximum effectivehalf diameter of the image-side surface of the first lens is denoted byEHD12, the maximum effective half diameter of the object-side surface ofthe second lens is denoted by EHD21, the maximum effective half diameterof the image-side surface of the second lens is denoted by EHD22, and soon.

The lens parameter related to an arc length of the shape of a surfaceand a surface profile:

For any surface of any lens, a profile curve length of the maximumeffective half diameter is, by definition, measured from a start pointwhere the optical axis of the belonging optical image capturing systempasses through the surface of the lens, along a surface profile of thelens, and finally to an end point of the maximum effective half diameterthereof. In other words, the curve length between the aforementionedstart and end points is the profile curve length of the maximumeffective half diameter, which is denoted by ARS. For example, theprofile curve length of the maximum effective half diameter of theobject-side surface of the first lens is denoted by ARS11, the profilecurve length of the maximum effective half diameter of the image-sidesurface of the first lens is denoted by ARS12, the profile curve lengthof the maximum effective half diameter of the object-side surface of thesecond lens is denoted by ARS21, the profile curve length of the maximumeffective half diameter of the image-side surface of the second lens isdenoted by ARS22, and so on.

For any surface of any lens, a profile curve length of a half of theentrance pupil diameter (HEP) is, by definition, measured from a startpoint where the optical axis of the belonging optical image capturingsystem passes through the surface of the lens, along a surface profileof the lens, and finally to a coordinate point of a perpendiculardistance where is a half of the entrance pupil diameter away from theoptical axis. In other words, the curve length between theaforementioned stat point and the coordinate point is the profile curvelength of a half of the entrance pupil diameter (HEP), and is denoted byARE. For example, the profile curve length of a half of the entrancepupil diameter (HEP) of the object-side surface of the first lens isdenoted by ARE11, the profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the first lens isdenoted by ARE12, the profile curve length of a half of the entrancepupil diameter (HEP) of the object-side surface of the second lens isdenoted by ARE21, the profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the second lens isdenoted by ARE22, and so on.

The lens parameter related to a depth of the lens shape:

A displacement from a point on the object-side surface of the seventhlens, which is passed through by the optical axis, to a point on theoptical axis, where a projection of the maximum effective semi diameterof the object-side surface of the seventh lens ends, is denoted byInRS71 (the depth of the maximum effective semi diameter). Adisplacement from a point on the image-side surface of the seventh lens,which is passed through by the optical axis, to a point on the opticalaxis, where a projection of the maximum effective semi diameter of theimage-side surface of the seventh lens ends, is denoted by InRS72 (thedepth of the maximum effective semi diameter). The depth of the maximumeffective semi diameter (sinkage) on the object-side surface or theimage-side surface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens,and the tangent point is tangent to a plane perpendicular to the opticalaxis and the tangent point cannot be a crossover point on the opticalaxis. By the definition, a distance perpendicular to the optical axisbetween a critical point C51 on the object-side surface of the fifthlens and the optical axis is HVT51 (instance), and a distanceperpendicular to the optical axis between a critical point C52 on theimage-side surface of the fifth lens and the optical axis is HVT52(instance). A distance perpendicular to the optical axis between acritical point C61 on the object-side surface of the sixth lens and theoptical axis is HVT61 (instance), and a distance perpendicular to theoptical axis between a critical point C62 on the image-side surface ofthe sixth lens and the optical axis is HVT62 (instance). A distanceperpendicular to the optical axis between a critical point on theobject-side or image-side surface of other lenses, e.g., the seventhlens, and the optical axis is denoted in the same manner.

The object-side surface of the seventh lens has one inflection pointIF711 which is nearest to the optical axis, and the sinkage value of theinflection point IF711 is denoted by SGI711 (instance). A distanceperpendicular to the optical axis between the inflection point IF711 andthe optical axis is HIF711 (instance). The image-side surface of theseventh lens has one inflection point IF721 which is nearest to theoptical axis, and the sinkage value of the inflection point IF721 isdenoted by SGI721 (instance). A distance perpendicular to the opticalaxis between the inflection point IF721 and the optical axis is HIF721(instance).

The object-side surface of the seventh lens has one inflection pointIF712 which is the second nearest to the optical axis, and the sinkagevalue of the inflection point IF712 is denoted by SGI712 (instance). Adistance perpendicular to the optical axis between the inflection pointIF712 and the optical axis is HIF712 (instance). The image-side surfaceof the seventh lens has one inflection point IF722 which is the secondnearest to the optical axis, and the sinkage value of the inflectionpoint IF722 is denoted by SGI722 (instance). A distance perpendicular tothe optical axis between the inflection point IF722 and the optical axisis HIF722 (instance).

The object-side surface of the seventh lens has one inflection pointIF713 which is the third nearest to the optical axis, and the sinkagevalue of the inflection point IF713 is denoted by SGI713 (instance). Adistance perpendicular to the optical axis between the inflection pointIF713 and the optical axis is HIF713 (instance). The image-side surfaceof the seventh lens has one inflection point IF723 which is the thirdnearest to the optical axis, and the sinkage value of the inflectionpoint IF723 is denoted by SGI723 (instance). A distance perpendicular tothe optical axis between the inflection point IF723 and the optical axisis HIF723 (instance).

The object-side surface of the seventh lens has one inflection pointIF714 which is the fourth nearest to the optical axis, and the sinkagevalue of the inflection point IF714 is denoted by SGI714 (instance). Adistance perpendicular to the optical axis between the inflection pointIF714 and the optical axis is HIF714 (instance). The image-side surfaceof the seventh lens has one inflection point IF724 which is the fourthnearest to the optical axis, and the sinkage value of the inflectionpoint IF724 is denoted by SGI724 (instance). A distance perpendicular tothe optical axis between the inflection point IF724 and the optical axisis HIF724 (instance).

An inflection point, a distance perpendicular to the optical axisbetween the inflection point and the optical axis, and a sinkage valuethereof on the object-side surface or image-side surface of other lensesis denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100% field. An offset of the spherical aberration is denoted by DFS.An offset of the coma aberration is denoted by DFC.

Transverse aberration on an edge of an aperture is denoted by STA, whichstands for STOP transverse aberration, and is used to evaluate theperformance of one specific optical image capturing system. Thetransverse aberration of light in any field of view can be calculatedwith a tangential fan or a sagittal fan. More specifically, thetransverse aberration caused when the longest operation wavelength(e.g., 650 nm) and the shortest operation wavelength (e.g., 470 nm) passthrough the edge of the aperture can be used as the reference forevaluating performance. The coordinate directions of the aforementionedtangential fan can be further divided into a positive direction (upperlight) and a negative direction (lower light). The longest operationwavelength which passes through the edge of the aperture has an imagingposition on the image plane in a particular field of view, and thereference wavelength of the mail light (e.g., 555 nm) has anotherimaging position on the image plane in the same field of view. Thetransverse aberration caused when the longest operation wavelengthpasses through the edge of the aperture is defined as a distance betweenthese two imaging positions. Similarly, the shortest operationwavelength which passes through the edge of the aperture has an imagingposition on the image plane in a particular field of view, and thetransverse aberration caused when the shortest operation wavelengthpasses through the edge of the aperture is defined as a distance betweenthe imaging position of the shortest operation wavelength and theimaging position of the reference wavelength. The performance of theoptical image capturing system can be considered excellent if thetransverse aberrations of the shortest and the longest operationwavelength which pass through the edge of the aperture and image on theimage plane in 0.7 field of view (i.e., 0.7 times the height for imageformation HOI) are both less than 100 μm. Furthermore, for a stricterevaluation, the performance cannot be considered excellent unless thetransverse aberrations of the shortest and the longest operationwavelength which pass through the edge of the aperture and image on theimage plane in 0.7 field of view are both less than 80 μm.

The optical image capturing system has a maximum image height HOI on theimage plane vertical to the optical axis. A transverse aberration at 0.7HOI in the positive direction of the tangential fan after the longestoperation wavelength of visible light passing through the edge of theaperture is denoted by PLTA; a transverse aberration at 0.7 HOI in thepositive direction of the tangential fan after the shortest operationwavelength of visible light passing through the edge of the aperture isdenoted by PSTA; a transverse aberration at 0.7 HOI in the negativedirection of the tangential fan after the longest operation wavelengthof visible light passing through the edge of the aperture is denoted byNLTA; a transverse aberration at 0.7 HOI in the negative direction ofthe tangential fan after the shortest operation wavelength of visiblelight passing through the edge of the aperture is denoted by NSTA; atransverse aberration at 0.7 HOI of the sagittal fan after the longestoperation wavelength of visible light passing through the edge of theaperture is denoted by SLTA; a transverse aberration at 0.7 HOI of thesagittal fan after the shortest operation wavelength of visible lightpassing through the edge of the aperture is denoted by SSTA.

The present invention provides an optical image capturing system capableof focusing visible and infrared light (i.e., dual-mode) at the sametime and achieving certain performance, in which the seventh lens isprovided with an inflection point at the object-side surface or at theimage-side surface to adjust the incident angle of each view field andmodify the ODT and the TDT. In addition, the surfaces of the seventhlens are capable of modifying the optical path to improve the imaginingquality.

The optical image capturing system of the present invention includes afirst lens, a second lens, a third lens, a fourth lens, a fifth lens, assixth lens, a seventh lens, a first image plane, and a second imageplane. The first image plane is an image plane specifically for thevisible light, and the first image plane is perpendicular to the opticalaxis; the through-focus modulation transfer rate (value of MTF) at thefirst spatial frequency has a maximum value at the central field of viewof the first image plane; the second image plane is an image planespecifically for the infrared light, and second image plane isperpendicular to the optical axis; the through-focus modulation transferrate (value of MTF) at the first spatial frequency has a maximum valueat the central of field of view of the second image plane. All lensesamong the first lens to the seventh lens have refractive power. Theoptical image capturing system satisfies:

1≤f/HEP≤10; 0 deg<HAF≤150 deg; and |FS|≤60 μm;

where f1, f2, f3, f4, f5, f6, and f7 are the focal lengths of the first,the second, the third, the fourth, the fifth, the sixth, the seventhlenses, respectively; f is a focal length of the optical image capturingsystem; HEP is an entrance pupil diameter of the optical image capturingsystem; HOS is a distance between the object-side surface of the firstlens and the first image plane on the optical axis; HAF is a half of amaximum view angle of the optical image capturing system; HOI is themaximum image height on the first image plane perpendicular to theoptical axis of the optical image capturing system; FS is the distanceon the optical axis between the first image plane and the second imageplane.

The present invention further provides an optical image capturingsystem, including a first lens, a second lens, a third lens, a fourthlens, a fifth lens, a sixth lens, a seventh lens, a first image plane,and a second image plane. The first image plane is an image planespecifically for the visible light, and the first image plane isperpendicular to the optical axis; the through-focus modulation transferrate (value of MTF) at the first spatial frequency has a maximum valueat the central field of view of the first image plane; the second imageplane is an image plane specifically for the infrared light, and secondimage plane is perpendicular to the optical axis; the through-focusmodulation transfer rate (value of MTF) at the first spatial frequencyhas a maximum value at the central of field of view of the second imageplane. The first lens has refractive power, and the object-side surfacethereof can be convex near the optical axis. The second lens hasrefractive power. The third lens has refractive power. The fourth lenshas refractive power. The fifth lens has refractive power. The sixthlens has refractive power. The seventh lens has refractive power. HOI isa maximum height for image formation perpendicular to the optical axison the image plane. At least one lens among the first lens to theseventh lens has positive refractive power. The optical image capturingsystem satisfies:

1≤f/HEP≤10; 0 deg<HAF≤150 deg; 0.9≤2(ARE/HEP)≤2.0; and

|FS|≤60 μm;

where f1, f2, f3, f4, f5, f6, and f7 are the focal lengths of the first,the second, the third, the fourth, the fifth, the sixth, the seventhlenses, respectively; f is a focal length of the optical image capturingsystem; HEP is an entrance pupil diameter of the optical image capturingsystem; HOS is a distance between the object-side surface of the firstlens and the first image plane on the optical axis; HAF is a half of amaximum view angle of the optical image capturing system; HOI is themaximum image height on the first image plane perpendicular to theoptical axis of the optical image capturing system; FS is the distanceon the optical axis between the first image plane and the second imageplane; ARE is a profile curve length measured from a start point wherethe optical axis of the belonging optical image capturing system passesthrough the surface of the lens, along a surface profile of the lens,and finally to a coordinate point of a perpendicular distance where is ahalf of the entrance pupil diameter away from the optical axis. At leastone lens among the first lens to the seventh lens is made of glass.

The present invention further provides an optical image capturingsystem, including a first lens, a second lens, a third lens, a fourthlens, a fifth lens, a sixth lens, a seventh lens, a first average imageplane, and a second average image plane. The first average image planeis an image plane specifically for the visible light, and the firstaverage image plane is perpendicular to the optical axis. The firstaverage image plane is installed at the average position of thedefocusing positions, where the values of MTF of the visible light atthe central field of view, 0.3 field of view, and the 0.7 field of vieware at their respective maximum at the first spatial frequency. Thesecond average image plane is an image plane specifically for theinfrared light, and the second average image plane is perpendicular tothe optical axis. The second average image plane is installed at theaverage position of the defocusing positions, where the values of MTF ofthe infrared light at the central field of view, 0.3 field of view, andthe 0.7 field of view are at their respective maximum at the firstspatial frequency. The number of the lenses having refractive power inthe optical image capturing system is seven. HOI is a maximum height forimage formation perpendicular to the optical axis on the image plane. Atleast one lens among the first lens to the seventh lens is made ofglass. The first lens has refractive power. The second lens hasrefractive power. The third lens has refractive power. The fourth lenshas refractive power. The fifth lens has refractive power. The sixthlens has refractive power. The seventh lens has refractive power. Atleast one lens among the first lens to the seventh lens has positiverefractive power. The optical image capturing system satisfies:

1≤f/HEP≤10; 0 deg<HAF≤150 deg; 0.9≤2(ARE/HEP)≤2.0; and

|AFS|≤60 μm;

where f1, f2, f3, f4, f5, f6, and f7 are the focal lengths of the first,the second, the third, the fourth, the fifth, the sixth, the seventhlenses, respectively; f is a focal length of the optical image capturingsystem; HEP is an entrance pupil diameter of the optical image capturingsystem; HOS is a distance between the object-side surface of the firstlens and the first average image plane on the optical axis; HAF is ahalf of a maximum view angle of the optical image capturing system; HOIis the maximum image height on the first average image planeperpendicular to the optical axis of the optical image capturing system;ARE is a profile curve length measured from a start point where theoptical axis of the belonging optical image capturing system passesthrough the surface of the lens, along a surface profile of the lens,and finally to a coordinate point of a perpendicular distance where is ahalf of the entrance pupil diameter away from the optical axis; AFS isthe distance between the first average image plane and the secondaverage image plane. At least one lens among the first lens to theseventh lens is made of glass.

For any surface of any lens, the profile curve length within theeffective half diameter affects the ability of the surface to correctaberration and differences between optical paths of light in differentfields of view. With longer profile curve length, the ability to correctaberration is better. However, the difficulty of manufacturing increasesas well. Therefore, the profile curve length within the effective halfdiameter of any surface of any lens has to be controlled. The ratiobetween the profile curve length (ARS) within the effective halfdiameter of one surface and the thickness (TP) of the lens, which thesurface belonged to, on the optical axis (i.e., ARS/TP) has to beparticularly controlled. For example, the profile curve length of themaximum effective half diameter of the object-side surface of the firstlens is denoted by ARS11, the thickness of the first lens on the opticalaxis is TP1, and the ratio between these two parameters is ARS11/TP1;the profile curve length of the maximum effective half diameter of theimage-side surface of the first lens is denoted by ARS12, and the ratiobetween ARS12 and TP1 is ARS12/TP1. The profile curve length of themaximum effective half diameter of the object-side surface of the secondlens is denoted by ARS21, the thickness of the second lens on theoptical axis is TP2, and the ratio between these two parameters isARS21/TP2; the profile curve length of the maximum effective halfdiameter of the image-side surface of the second lens is denoted byARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. For any surfaceof other lenses in the optical image capturing system, the ratio betweenthe profile curve length of the maximum effective half diameter thereofand the thickness of the lens which the surface belonged to is denotedin the same manner.

For any surface of any lens, the profile curve length within a half ofthe entrance pupil diameter (HEP) affects the ability of the surface tocorrect aberration and differences between optical paths of light indifferent fields of view. With longer profile curve length, the abilityto correct aberration is better. However, the difficulty ofmanufacturing increases as well. Therefore, the profile curve lengthwithin a half of the entrance pupil diameter (HEP) of any surface of anylens has to be controlled. The ratio between the profile curve length(ARE) within a half of the entrance pupil diameter (HEP) of one surfaceand the thickness (TP) of the lens, which the surface belonged to, onthe optical axis (i.e., ARE/TP) has to be particularly controlled. Forexample, the profile curve length of a half of the entrance pupildiameter (HEP) of the object-side surface of the first lens is denotedby ARE11, the thickness of the first lens on the optical axis is TP1,and the ratio between these two parameters is ARE11/TP1; the profilecurve length of a half of the entrance pupil diameter (HEP) of theimage-side surface of the first lens is denoted by ARE12, and the ratiobetween ARE12 and TP1 is ARE12/TP1. The profile curve length of a halfof the entrance pupil diameter (HEP) of the object-side surface of thesecond lens is denoted by ARE21, the thickness of the second lens on theoptical axis is TP2, and the ratio between these two parameters isARE21/TP2; the profile curve length of a half of the entrance pupildiameter (HEP) of the image-side surface of the second lens is denotedby ARE22, and the ratio between ARE22 and TP2 is ARE22/TP2. For anysurface of other lenses in the optical image capturing system, the ratiobetween the profile curve length of a half of the entrance pupildiameter (HEP) thereof and the thickness of the lens which the surfacebelonged to is denoted in the same manner.

In an embodiment, a height of the optical image capturing system (HOS)can be reduced while |f1|>f7.

In an embodiment, when |f2|+|f3|+|f4|+|f5|+|f6| and |f1|+|f7| of thelenses satisfy the aforementioned conditions, at least one lens amongthe second to the sixth lenses could have weak positive refractive poweror weak negative refractive power. Herein the weak refractive powermeans the absolute value of the focal length of one specific lens isgreater than 10. When at least one lens among the second to the sixthlenses has weak positive refractive power, it may share the positiverefractive power of the first lens, and on the contrary, when at leastone lens among the second to the sixth lenses has weak negativerefractive power, it may fine turn and correct the aberration of thesystem.

In an embodiment, the seventh lens could have negative refractive power,and an image-side surface thereof is concave, it may reduce back focallength and size. Besides, the seventh lens can have at least aninflection point on at least a surface thereof, which may reduce anincident angle of the light of an off-axis field of view and correct theaberration of the off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to thefollowing detailed description of some illustrative embodiments inconjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the presentinvention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the first embodiment of thepresent application;

FIG. 1C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the first embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 1D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the first embodiment of the present invention;

FIG. 1E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the first embodiment of the present disclosure;

FIG. 2A is a schematic diagram of a second embodiment of the presentinvention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the second embodiment of thepresent application;

FIG. 2C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the second embodiment of the present application,and a transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 2D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the second embodiment of the present invention;

FIG. 2E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the second embodiment of the presentdisclosure;

FIG. 3A is a schematic diagram of a third embodiment of the presentinvention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the third embodiment of thepresent application;

FIG. 3C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the third embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 3D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the third embodiment of the present invention;

FIG. 3E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the third embodiment of the present disclosure;

FIG. 4A is a schematic diagram of a fourth embodiment of the presentinvention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the fourth embodiment of thepresent application;

FIG. 4C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the fourth embodiment of the present application,and a transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 4D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the fourth embodiment of the present invention;

FIG. 4E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the fourth embodiment of the presentdisclosure;

FIG. 5A is a schematic diagram of a fifth embodiment of the presentinvention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the fifth embodiment of thepresent application;

FIG. 5C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the fifth embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 5D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the fifth embodiment of the present invention;

FIG. 5E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the fifth embodiment of the present disclosure;

FIG. 6A is a schematic diagram of a sixth embodiment of the presentinvention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the sixth embodiment of thepresent application;

FIG. 6C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the sixth embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 6D is a diagram showing the through-focus MTF values of the visiblelight spectrum at the central field of view, 0.3 field of view, and 0.7field of view of the sixth embodiment of the present invention; and

FIG. 6E is a diagram showing the through-focus MTF values of theinfrared light spectrum at the central field of view, 0.3 field of view,and 0.7 field of view of the sixth embodiment of the present disclosure.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes afirst lens, a second lens, a third lens, a fourth lens, a fifth lens, asixth lens, a seventh lens, and an image plane from an object side to animage side. The optical image capturing system further is provided withan image sensor at an image plane. The height for image formation ineach of the following embodiments is about 3.91 mm.

The optical image capturing system can work in three wavelengths,including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the mainreference wavelength and is the reference wavelength for obtaining thetechnical characters. The optical image capturing system can also workin five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650nm wherein 555 nm is the main reference wavelength, and is the referencewavelength for obtaining the technical characters.

The optical image capturing system of the present invention satisfies0.5≤ΣPPR/|ΣNPR|≤15, and a preferable range is 1≤ΣPPR/|ΣNPR|≤3.0, wherePPR is a ratio of the focal length fp of the optical image capturingsystem to a focal length fp of each of lenses with positive refractivepower; NPR is a ratio of the focal length fn of the optical imagecapturing system to a focal length fn of each of lenses with negativerefractive power; ΣPPR is a sum of the PPRs of each positive lens; andΣNPR is a sum of the NPRs of each negative lens. It is helpful forcontrol of an entire refractive power and an entire length of theoptical image capturing system.

The image sensor is provided on the image plane. The optical imagecapturing system of the present invention satisfies HOS/HOI≤10 and0.5≤HOS/f≤10, and a preferable range is 1≤HOS/HOI≤5 and 1≤HOS/f≤7, whereHOI is a half of a diagonal of an effective sensing area of the imagesensor, i.e., the maximum image height, and HOS is a height of theoptical image capturing system, i.e. a distance on the optical axisbetween the object-side surface of the first lens and the image plane.It is helpful for reduction of the size of the system for used incompact cameras.

The optical image capturing system of the present invention further isprovided with an aperture to increase image quality.

In the optical image capturing system of the present invention, theaperture could be a front aperture or a middle aperture, wherein thefront aperture is provided between the object and the first lens, andthe middle is provided between the first lens and the image plane. Thefront aperture provides a long distance between an exit pupil of thesystem and the image plane, which allows more elements to be installed.The middle could enlarge a view angle of view of the system and increasethe efficiency of the image sensor. The optical image capturing systemsatisfies 0.2≤InS/HOS≤1.1, where InS is a distance between the apertureand the image-side surface of the sixth lens. It is helpful for sizereduction and wide angle.

The optical image capturing system of the present invention satisfies0.1≤ΣTP/InTL≤0.9, where InTL is a distance between the object-sidesurface of the first lens and the image-side surface of the seventhlens, and ΣTP is a sum of central thicknesses of the lenses on theoptical axis. It is helpful for the contrast of image and yield rate ofmanufacture and provides a suitable back focal length for installationof other elements.

The optical image capturing system of the present invention satisfies0.001≤|R1/R2|≤20, and a preferable range is 0.01≤|R1/R2|<10, where R1 isa radius of curvature of the object-side surface of the first lens, andR2 is a radius of curvature of the image-side surface of the first lens.It provides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies−7<(R11−R12)/(R11+R12)<50, where R13 is a radius of curvature of theobject-side surface of the seventh lens, and R14 is a radius ofcurvature of the image-side surface of the seventh lens. It may modifythe astigmatic field curvature.

The optical image capturing system of the present invention satisfiesIN12/f≤3.0, where IN12 is a distance on the optical axis between thefirst lens and the second lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing system of the present invention satisfiesIN67/f≤0.8, where IN67 is a distance on the optical axis between thesixth lens and the seventh lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing system of the present invention satisfies0.1≤(TP1+IN12)/TP2≤10, where TP1 is a central thickness of the firstlens on the optical axis, and TP2 is a central thickness of the secondlens on the optical axis. It may control the sensitivity of manufactureof the system and improve the performance.

The optical image capturing system of the present invention satisfies0.1≤(TP7+IN67)/TP6≤10, where TP6 is a central thickness of the sixthlens on the optical axis, TP7 is a central thickness of the seventh lenson the optical axis, and IN67 is a distance between the sixth lens andthe seventh lens. It may control the sensitivity of manufacture of thesystem and improve the performance.

The optical image capturing system of the present invention satisfies0.1≤TP4/(IN34+TP4+IN45)<1, where TP3 is a central thickness of the thirdlens on the optical axis, TP4 is a central thickness of the fourth lenson the optical axis, TP5 is a central thickness of the fifth lens on theoptical axis, IN34 is a distance on the optical axis between the thirdlens and the fourth lens, IN45 is a distance on the optical axis betweenthe fourth lens and the fifth lens, and InTL is a distance between theobject-side surface of the first lens and the image-side surface of theseventh lens. It may fine tune and correct the aberration of theincident rays layer by layer, and reduce the height of the system.

The optical image capturing system satisfies 0 mm≤HVT71≤3 mm; 0mm<HVT72≤6 mm; 0≤HVT71/HVT72; 0 mm≤|SGC71|≤0.5 mm; 0 mm<|SGC72|≤2 mm;and 0<|SGC72|/(|SGC72|+TP7)≤0.9, where HVT71 a distance perpendicular tothe optical axis between the critical point C71 on the object-sidesurface of the seventh lens and the optical axis; HVT72 a distanceperpendicular to the optical axis between the critical point C72 on theimage-side surface of the seventh lens and the optical axis; SGC71 is adistance on the optical axis between a point on the object-side surfaceof the seventh lens where the optical axis passes through and a pointwhere the critical point C71 projects on the optical axis; SGC72 is adistance on the optical axis between a point on the image-side surfaceof the seventh lens where the optical axis passes through and a pointwhere the critical point C72 projects on the optical axis. It is helpfulto correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≤HVT72/HOI≤0.9, andpreferably satisfies 0.3≤HVT72/HOI≤0.8. It may help to correct theperipheral aberration.

The optical image capturing system satisfies 0≤HVT72/HOS≤0.5, andpreferably satisfies 0.2≤HVT72/HOS≤0.45. It may help to correct theperipheral aberration.

The optical image capturing system of the present invention satisfies0<SGI711/(SGI711+TP7)≤0.9; 0<SGI721/(SGI721+TP7)≤0.9, and it ispreferable to satisfy 0.1≤SGI711/(SGI711+TP7)≤0.6;0.1≤SGI721/(SGI721+TP7)≤0.6, where SGI711 is a displacement on theoptical axis from a point on the object-side surface of the seventhlens, through which the optical axis passes, to a point where theinflection point on the object-side surface, which is the closest to theoptical axis, projects on the optical axis, and SGI721 is a displacementon the optical axis from a point on the image-side surface of theseventh lens, through which the optical axis passes, to a point wherethe inflection point on the image-side surface, which is the closest tothe optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies0<SGI712/(SGI712+TP7)≤0.9; 0<SGI722/(SGI722+TP7)≤0.9, and it ispreferable to satisfy 0.1≤SGI712/(SGI712+TP7)≤0.6;0.1≤SGI722/(SGI722+TP7)≤0.6, where SGI712 is a displacement on theoptical axis from a point on the object-side surface of the seventhlens, through which the optical axis passes, to a point where theinflection point on the object-side surface, which is the second closestto the optical axis, projects on the optical axis, and SGI722 is adisplacement on the optical axis from a point on the image-side surfaceof the seventh lens, through which the optical axis passes, to a pointwhere the inflection point on the image-side surface, which is thesecond closest to the optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF711|≤5 mm; 0.001 mm≤|HIF721|≤5 mm, and it is preferable tosatisfy 0.1 mm≤HIF711|≤3.5 mm; 1.5 mm≤|HIF721|≤3.5 mm, where HIF711 is adistance perpendicular to the optical axis between the inflection pointon the object-side surface of the seventh lens, which is the closest tothe optical axis, and the optical axis; HIF721 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the seventh lens, which is the closest to theoptical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF712|≤5 mm; 0.001 mm≤|HIF722|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF722|≤3.5 mm; 0.1 mm≤|HIF712|≤3.5 mm, where HIF712 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is thesecond closest to the optical axis, and the optical axis; HIF722 is adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the seventh lens, which is the secondclosest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF713|≤5 mm; 0.001 mm≤|HIF723|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF723|≤3.5 mm; 0.1 mm≤|HIF713|≤3.5 mm, where HIF713 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is the thirdclosest to the optical axis, and the optical axis; HIF723 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the seventh lens, which is the third closest tothe optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF714|≤5 mm; 0.001 mm≤|HIF724|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF724|≤3.5 mm; 0.1 mm≤|HIF714|≤3.5 mm, where HIF714 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is thefourth closest to the optical axis, and the optical axis; HIF724 is adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the seventh lens, which is the fourthclosest to the optical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of lowAbbe number are arranged in an interlaced arrangement that could behelpful for correction of aberration of the system.

An equation of aspheric surface is

z=ch ²/[1+[1(k+l)c ² h ²]^(0.5) ]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .  (1)

where z is a depression of the aspheric surface; k is conic constant; cis reciprocal of the radius of curvature; and A4, A6, A8, A10, A12, A14,A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made ofplastic or glass. The plastic lenses may reduce the weight and lower thecost of the system, and the glass lenses may control the thermal effectand enlarge the space for arrangement of the refractive power of thesystem. In addition, the opposite surfaces (object-side surface andimage-side surface) of the first to the seventh lenses could be asphericthat can obtain more control parameters to reduce aberration. The numberof aspheric glass lenses could be less than the conventional sphericalglass lenses, which is helpful for reduction of the height of thesystem.

When the lens has a convex surface, which means that the surface isconvex around a position, through which the optical axis passes, andwhen the lens has a concave surface, which means that the surface isconcave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could beapplied in a dynamic focusing optical system. It is superior in thecorrection of aberration and high imaging quality so that it could beallied in lots of fields.

The optical image capturing system of the present invention couldfurther include a driving module to meet different demands, wherein thedriving module can be coupled with the lenses to move the lenses. Thedriving module can be a voice coil motor (VCM), which is used to movethe lens for focusing, or can be an optical image stabilization (OIS)component, which is used to lower the possibility of having the problemof image blurring which is caused by subtle movements of the lens whileshooting.

To meet different requirements, at least one lens among the first lensto the seventh lens of the optical image capturing system of the presentinvention can be a light filter, which filters out light of wavelengthshorter than 500 nm. Such effect can be achieved by coating on at leastone surface of the lens, or by using materials capable of filtering outshort waves to make the lens.

To meet different requirements, the image plane of the optical imagecapturing system in the present invention can be either flat or curved.If the image plane is curved (e.g., a sphere with a radius ofcurvature), the incidence angle required for focusing light on the imageplane can be decreased, which is not only helpful to shorten the lengthof the system (TTL), but also helpful to increase the relativeilluminance.

We provide several embodiments in conjunction with the accompanyingdrawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 ofthe first embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 110, an aperture100, a second lens 120, a third lens 130, a fourth lens 140, a fifthlens 150, a sixth lens 160, a seventh lens 170, an infrared rays filter180, an image plane 190, and an image sensor 192. FIG. 1C shows atangential fan and a sagittal fan of the optical image capturing system10 of the first embodiment of the present application, and a transverseaberration diagram at 0.7 field of view when a longest operationwavelength and a shortest operation wavelength pass through an edge ofthe aperture 100. FIG. 1D is a diagram showing the through-focus MTFvalues of the visible light spectrum at the central field of view, 0.3field of view, and 0.7 field of view of the first embodiment of thepresent invention. FIG. 1E is a diagram showing the through-focus MTFvalues of the infrared light spectrum at the central field of view, 0.3field of view, and 0.7 field of view of the first embodiment of thepresent disclosure.

The first lens 110 has negative refractive power and is made of plastic.An object-side surface 112 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 114 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 112 has an inflection point thereon, and the image-side surface114 has two inflection points. A profile curve length of the maximumeffective half diameter of an object-side surface of the first lens 110is denoted by ARS11, and a profile curve length of the maximum effectivehalf diameter of the image-side surface of the first lens 110 is denotedby ARS12. A profile curve length of a half of an entrance pupil diameter(HEP) of the object-side surface of the first lens 110 is denoted byARE11, and a profile curve length of a half of the entrance pupildiameter (HEP) of the image-side surface of the first lens 110 isdenoted by ARE12. A thickness of the first lens 110 on the optical axisis TP1.

The first lens satisfies SGI111=−0.1110 mm; SGI121=2.7120 mm; TP1=2.2761mm; |SGI111|/(|SGI111|+TP1)=0.0465; |SGI121|/(|SGI121|+TP1)=0.5437,where SGI111 is a displacement on the optical axis from a point on theobject-side surface of the first lens, through which the optical axispasses, to a point where the inflection point on the object-sidesurface, which is the closest to the optical axis, projects on theoptical axis, and SGI121 is a displacement on the optical axis from apoint on the image-side surface of the first lens, through which theoptical axis passes, to a point where the inflection point on theimage-side surface, which is the closest to the optical axis, projectson the optical axis.

The first lens satisfies SGI112=0 mm; SGI122=4.2315 mm;|SGI112|/(|SGI112|+TP1)=0; |SGI122|/(|SGI122|+TP1)=0.6502, where SGI112is a displacement on the optical axis from a point on the object-sidesurface of the first lens, through which the optical axis passes, to apoint where the inflection point on the object-side surface, which isthe second closest to the optical axis, projects on the optical axis,and SGI121 is a displacement on the optical axis from a point on theimage-side surface of the first lens, through which the optical axispasses, to a point where the inflection point on the image-side surface,which is the second closest to the optical axis, projects on the opticalaxis.

The first lens satisfies HIF111=12.8432 mm; HIF111/HOI=1.7127;HIF121=7.1744 mm; HIF121/HOI=0.9567, where HIF111 is a displacementperpendicular to the optical axis from a point on the object-sidesurface of the first lens, through which the optical axis passes, to theinflection point, which is the closest to the optical axis; HIF121 is adisplacement perpendicular to the optical axis from a point on theimage-side surface of the first lens, through which the optical axispasses, to the inflection point, which is the closest to the opticalaxis.

The first lens satisfies HIF112=0 mm; HIF112/HOI=0; HIF122=9.8592 mm;HIF122/HOI=1.3147, where HIF112 is a displacement perpendicular to theoptical axis from a point on the object-side surface of the first lens,through which the optical axis passes, to the inflection point, which isthe second closest to the optical axis; HIF122 is a displacementperpendicular to the optical axis from a point on the image-side surfaceof the first lens, through which the optical axis passes, to theinflection point, which is the second closest to the optical axis.

The second lens 120 has positive refractive power and is made ofplastic. An object-side surface 122 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 124thereof, which faces the image side, is a concave aspheric surface. Aprofile curve length of the maximum effective half diameter of anobject-side surface of the second lens 120 is denoted by ARS21, and aprofile curve length of the maximum effective half diameter of theimage-side surface of the second lens 120 is denoted by ARS22. A profilecurve length of a half of an entrance pupil diameter (HEP) of theobject-side surface of the second lens 120 is denoted by ARE21, and aprofile curve length of a half of the entrance pupil diameter (HEP) ofthe image-side surface of the second lens 120 is denoted by ARE22. Athickness of the second lens 120 on the optical axis is TP2.

For the second lens, a displacement on the optical axis from a point onthe object-side surface of the second lens, through which the opticalaxis passes, to a point where the inflection point on the image-sidesurface, which is the closest to the optical axis, projects on theoptical axis, is denoted by SGI211, and a displacement on the opticalaxis from a point on the image-side surface of the second lens, throughwhich the optical axis passes, to a point where the inflection point onthe image-side surface, which is the closest to the optical axis,projects on the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axisfrom a point on the object-side surface of the second lens, throughwhich the optical axis passes, to the inflection point, which is theclosest to the optical axis is denoted by HIF211, and a displacementperpendicular to the optical axis from a point on the image-side surfaceof the second lens, through which the optical axis passes, to theinflection point, which is the closest to the optical axis is denoted byHIF221.

The third lens 130 has negative refractive power and is made of plastic.An object-side surface 132, which faces the object side, is a convexaspheric surface, and an image-side surface 134, which faces the imageside, is a concave aspheric surface. A profile curve length of themaximum effective half diameter of an object-side surface of the thirdlens 130 is denoted by ARS31, and a profile curve length of the maximumeffective half diameter of the image-side surface of the third lens 130is denoted by ARS32. A profile curve length of a half of an entrancepupil diameter (HEP) of the object-side surface of the third lens 130 isdenoted by ARE31, and a profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the third lens 130 isdenoted by ARE32. A thickness of the third lens 130 on the optical axisis TP3.

For the third lens 130, SGI311 is a displacement on the optical axisfrom a point on the object-side surface of the third lens, through whichthe optical axis passes, to a point where the inflection point on theobject-side surface, which is the closest to the optical axis, projectson the optical axis, and SGI321 is a displacement on the optical axisfrom a point on the image-side surface of the third lens, through whichthe optical axis passes, to a point where the inflection point on theimage-side surface, which is the closest to the optical axis, projectson the optical axis.

For the third lens 130, SGI312 is a displacement on the optical axisfrom a point on the object-side surface of the third lens, through whichthe optical axis passes, to a point where the inflection point on theobject-side surface, which is the second closest to the optical axis,projects on the optical axis, and SGI322 is a displacement on theoptical axis from a point on the image-side surface of the third lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, projects on the optical axis.

For the third lens 130, HIF311 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe third lens, which is the closest to the optical axis, and theoptical axis; HIF321 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the thirdlens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe third lens, which is the second closest to the optical axis, and theoptical axis; HIF322 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the thirdlens, which is the second closest to the optical axis, and the opticalaxis.

The fourth lens 140 has positive refractive power and is made ofplastic. An object-side surface 142, which faces the object side, is aconvex aspheric surface, and an image-side surface 144, which faces theimage side, is a convex aspheric surface. The object-side surface 142has an inflection point. A profile curve length of the maximum effectivehalf diameter of an object-side surface of the fourth lens 140 isdenoted by ARS41, and a profile curve length of the maximum effectivehalf diameter of the image-side surface of the fourth lens 140 isdenoted by ARS42. A profile curve length of a half of an entrance pupildiameter (HEP) of the object-side surface of the fourth lens 140 isdenoted by ARE41, and a profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the fourth lens 140 isdenoted by ARE42. A thickness of the fourth lens 140 on the optical axisis TP4.

The fourth lens 140 satisfies SGI411=0.0018 mm;|SGI411|/(|SGI411|+TP4)=0.0009, where SGI411 is a displacement on theoptical axis from a point on the object-side surface of the fourth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, projects on the optical axis, and SGI421 is a displacement on theoptical axis from a point on the image-side surface of the fourth lens,through which the optical axis passes, to a point where the inflectionpoint on the image-side surface, which is the closest to the opticalaxis, projects on the optical axis.

For the fourth lens 140, SGI412 is a displacement on the optical axisfrom a point on the object-side surface of the fourth lens, throughwhich the optical axis passes, to a point where the inflection point onthe object-side surface, which is the second closest to the opticalaxis, projects on the optical axis, and SGI422 is a displacement on theoptical axis from a point on the image-side surface of the fourth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, projects on the optical axis.

The fourth lens 140 further satisfies HIF411=0.7191 mm;HIF411/HOI=0.0959, where HIF411 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fourth lens, which is the closest to the optical axis, and theoptical axis; HIF421 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fourthlens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fourth lens, which is the second closest to the optical axis, andthe optical axis; HIF422 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fourthlens, which is the second closest to the optical axis, and the opticalaxis.

The fifth lens 150 has positive refractive power and is made of plastic.An object-side surface 152, which faces the object side, is a concaveaspheric surface, and an image-side surface 154, which faces the imageside, is a convex aspheric surface. The object-side surface 152 and theimage-side surface 154 both have an inflection point. A profile curvelength of the maximum effective half diameter of an object-side surfaceof the fifth lens 150 is denoted by ARS51, and a profile curve length ofthe maximum effective half diameter of the image-side surface of thefifth lens 150 is denoted by ARS52. A profile curve length of a half ofan entrance pupil diameter (HEP) of the object-side surface of the fifthlens 150 is denoted by ARE51, and a profile curve length of a half ofthe entrance pupil diameter (HEP) of the image-side surface of the fifthlens 150 is denoted by ARE52. A thickness of the fifth lens 150 on theoptical axis is TP5.

The fifth lens 150 satisfies SGI511=−0.1246 mm; SGI521=−2.1477 mm;|SGI511|/(|SGI511|+TP5)=0.0284; |SGI521|/(|SGI521|+TP5)=0.3346, whereSGI511 is a displacement on the optical axis from a point on theobject-side surface of the fifth lens, through which the optical axispasses, to a point where the inflection point on the object-sidesurface, which is the closest to the optical axis, projects on theoptical axis, and SGI521 is a displacement on the optical axis from apoint on the image-side surface of the fifth lens, through which theoptical axis passes, to a point where the inflection point on theimage-side surface, which is the closest to the optical axis, projectson the optical axis.

For the fifth lens 150, SGI512 is a displacement on the optical axisfrom a point on the object-side surface of the fifth lens, through whichthe optical axis passes, to a point where the inflection point on theobject-side surface, which is the second closest to the optical axis,projects on the optical axis, and SGI522 is a displacement on theoptical axis from a point on the image-side surface of the fifth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, projects on the optical axis.

The fifth lens 150 further satisfies HIF511=3.8179 mm; HIF521=4.5480 mm;HIF511/HOI=0.5091; HIF521/HOI=0.6065, where HIF511 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the fifth lens, which is the closest to theoptical axis, and the optical axis; HIF521 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the fifth lens, which is the closest to the optical axis, andthe optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fifth lens, which is the second closest to the optical axis, and theoptical axis; HIF522 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fifthlens, which is the second closest to the optical axis, and the opticalaxis.

The sixth lens 160 has negative refractive power and is made of plastic.An object-side surface 162, which faces the object side, is a convexsurface, and an image-side surface 164, which faces the image side, is aconcave surface. The object-side surface 162 and the image-side surface164 both have an inflection point, which could adjust the incident angleof each view field to improve aberration. A profile curve length of themaximum effective half diameter of an object-side surface of the sixthlens 160 is denoted by ARS61, and a profile curve length of the maximumeffective half diameter of the image-side surface of the sixth lens 160is denoted by ARS62. A profile curve length of a half of an entrancepupil diameter (HEP) of the object-side surface of the sixth lens 160 isdenoted by ARE61, and a profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the sixth lens 160 isdenoted by ARE62. A thickness of the sixth lens 160 on the optical axisis TP6.

The sixth lens 160 satisfies SGI611=0.3208 mm; SGI621=0.5937 mm;|SGI611|/(|SGI611|+TP6)=0.5167; |SGI621|/(|SGI621|+TP6)=0.6643, whereSGI611 is a displacement on the optical axis from a point on theobject-side surface of the sixth lens, through which the optical axispasses, to a point where the inflection point on the object-sidesurface, which is the closest to the optical axis, projects on theoptical axis, and SGI621 is a displacement on the optical axis from apoint on the image-side surface of the sixth lens, through which theoptical axis passes, to a point where the inflection point on theimage-side surface, which is the closest to the optical axis, projectson the optical axis.

The sixth lens 160 further satisfies HIF611=1.9655 mm; HIF621=2.0041 mm;HIF611/HOI=0.2621; HIF621/HOI=0.2672, where HIF611 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the sixth lens, which is the closest to theoptical axis, and the optical axis; HIF621 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the sixth lens, which is the closest to the optical axis, andthe optical axis.

The seventh lens 170 has positive refractive power and is made ofplastic. An object-side surface 172, which faces the object side, is aconvex surface, and an image-side surface 174, which faces the imageside, is a concave surface. This would help to shorten the back focallength, whereby to keep the optical image capturing system miniaturized.The object-side surface 172 and the image-side surface 174 both have aninflection point. A profile curve length of the maximum effective halfdiameter of an object-side surface of the seventh lens 170 is denoted byARS71, and a profile curve length of the maximum effective half diameterof the image-side surface of the seventh lens 170 is denoted by ARS72. Aprofile curve length of a half of an entrance pupil diameter (HEP) ofthe object-side surface of the seventh lens 170 is denoted by ARE71, anda profile curve length of a half of the entrance pupil diameter (HEP) ofthe image-side surface of the seventh lens 170 is denoted by ARE72. Athickness of the seventh lens 170 on the optical axis is TP7.

The seventh lens 170 satisfies SGI711=0.5212 mm; SGI721=0.5668 mm;|SGI711|/(|SGI711|+TP7)=0.3179; |SGI721|/(|SGI721|+TP7)=0.3364, whereSGI711 is a displacement on the optical axis from a point on theobject-side surface of the seventh lens, through which the optical axispasses, to a point where the inflection point on the object-sidesurface, which is the closest to the optical axis, projects on theoptical axis, and SGI721 is a displacement on the optical axis from apoint on the image-side surface of the seventh lens, through which theoptical axis passes, to a point where the inflection point on theimage-side surface, which is the closest to the optical axis, projectson the optical axis.

The seventh lens 170 further satisfies HIF711=1.6707 mm; HIF721=1.8616mm; HIF711/HOI=0.2228; HIF721/HOI=0.2482, where HIF711 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the seventh lens, which is the closest to theoptical axis, and the optical axis; HIF721 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the seventh lens, which is the closest to the optical axis,and the optical axis.

The infrared rays filter 180 is made of glass and between the seventhlens 170 and the image plane 190. The infrared rays filter 180 gives nocontribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has thefollowing parameters, which are f=4.3019 mm; f/HEP=1.2; HAF=59.9968 deg;and tan(HAF)=1.7318, where f is a focal length of the system; HAF is ahalf of the maximum field angle; and HEP is an entrance pupil diameter.

The parameters of the lenses of the first embodiment are f1=−14.5286 mm;|f/f1|=0.2961; f7=8.2933; |f1|>f7; and |f1/f7|=1.7519, where f1 is afocal length of the first lens 110; and f7 is a focal length of theseventh lens 170.

The first embodiment further satisfies|f2|+|f3|+|f4|+|f5|+|f6|=144.7494; |f1|+|f7|=22.8219 and|f2|+|f3|+|f4|+|f5|+|f6|>|f1|+|f7|, where f2 is a focal length of thesecond lens 120, f3 is a focal length of the third lens 130, f4 is afocal length of the fourth lens 140, f5 is a focal length of the fifthlens 150, and f6 is a focal length of the sixth lens 160.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣPPR=f/f2+f/f4+f/f5+f/f7=1.7384; ΣNPR=f/f1+f/f3+f/f6=−0.9999;ΣPPR/|ΣNPR|=1.7386; |f/f2|=0.1774; |f/f3|=0.0443; |f/f4|=0.4411;|f/f5|=0.6012; |f/f6|=0.6595; |f/f7|=0.5187, where PPR is a ratio of afocal length fp of the optical image capturing system to a focal lengthfp of each of the lenses with positive refractive power; and NPR is aratio of a focal length fn of the optical image capturing system to afocal length fn of each of lenses with negative refractive power.

The optical image capturing system 10 of the first embodiment furthersatisfies InTL+BFL=HOS; HOS=26.9789 mm; HOI=7.5 mm; HOS/HOI=3.5977;HOS/f=6.2715; InS=12.4615 mm; and InS/HOS=0.4619, where InTL is adistance between the object-side surface 112 of the first lens 110 andthe image-side surface 174 of the seventh lens 170; HOS is a height ofthe image capturing system, i.e. a distance between the object-sidesurface 112 of the first lens 110 and the image plane 190; InS is adistance between the aperture 100 and the image plane 190; HOI is a halfof a diagonal of an effective sensing area of the image sensor 192,i.e., the maximum image height; and BFL is a distance between theimage-side surface 174 of the seventh lens 170 and the image plane 190.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣTP=16.0446 mm; and ΣTP/InTL=0.6559, where ΣTP is a sum of thethicknesses of the lenses 110-150 with refractive power. It is helpfulfor the contrast of image and yield rate of manufacture and provides asuitable back focal length for installation of other elements.

The optical image capturing system 10 of the first embodiment furthersatisfies |R1/R2|=129.9952, where R1 is a radius of curvature of theobject-side surface 112 of the first lens 110, and R2 is a radius ofcurvature of the image-side surface 114 of the first lens 110. Itprovides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment furthersatisfies (R13−R14)/(R13+R14)=−0.0806, where R13 is a radius ofcurvature of the object-side surface 172 of the seventh lens 170, andR14 is a radius of curvature of the image-side surface 174 of theseventh lens 170. It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣPP=f2+f4+f5+f7=49.4535 mm; and f4/(f2+f4+f5+f7)=0.1972, whereΣPP is a sum of the focal length fp of each lens with positiverefractive power. It is helpful to share the positive refractive powerof the fourth lens 140 to other positive lenses to avoid the significantaberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣNP=f1+f3+f6=−118.1178 mm; and f1/(f1+f3+f6)=0.1677, where ΣNPis a sum of the focal length fn of each lens with negative refractivepower. It is helpful to share the negative refractive power of the firstlens 110 to other negative lenses, which avoids the significantaberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment furthersatisfies IN12=4.5524 mm; IN12/f=1.0582, where IN12 is a distance on theoptical axis between the first lens 110 and the second lens 120. It maycorrect chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies TP1=2.2761 mm; TP2=0.2398 mm; and (TP1+IN12)/TP2=1.3032, whereTP1 is a central thickness of the first lens 110 on the optical axis,and TP2 is a central thickness of the second lens 120 on the opticalaxis. It may control the sensitivity of manufacture of the system andimprove the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies TP6=0.3000 mm; TP7=1.1182 mm; and (TP7+IN67)/TP6=4.4322, whereTP6 is a central thickness of the sixth lens 160 on the optical axis,TP7 is a central thickness of the seventh lens 170 on the optical axis,and IN67 is a distance on the optical axis between the sixth lens 160and the seventh lens 170. It may control the sensitivity of manufactureof the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment furthersatisfies TP3=0.8369 mm; TP4=2.0022 mm; TP5=4.2706 mm; IN34=1.9268 mm;IN45=1.5153 mm; and TP4/(IN34+TP4+IN45)=0.3678, where TP3 is a centralthickness of the third lens 130 on the optical axis, TP4 is a centralthickness of the fourth lens 140 on the optical axis, TP5 is a centralthickness of the fifth lens 150 on the optical axis, IN34 is a distanceon the optical axis between the third lens 130 and the fourth lens 140,IN45 is a distance on the optical axis between the fourth lens 140 andthe fifth lens 150, and InTL is a distance from the object-side surface112 of the first lens 110 to the image-side surface 174 of the seventhlens 170 on the optical axis. It may control the sensitivity ofmanufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment furthersatisfies InRS61=−0.7823 mm; InRS62=−0.2166 mm; and ∥InRS62|/TP6=0.722,where InRS61 is a displacement from a point on the object-side surface162 of the sixth lens 160 passed through by the optical axis to a pointon the optical axis where a projection of the maximum effective semidiameter of the object-side surface 162 of the sixth lens 160 ends;InRS62 is a displacement from a point on the image-side surface 166 ofthe sixth lens 160 passed through by the optical axis to a point on theoptical axis where a projection of the maximum effective semi diameterof the image-side surface 166 of the sixth lens 160 ends; and TP6 is acentral thickness of the sixth lens 160 on the optical axis. It ishelpful for manufacturing and shaping of the lenses and is helpful toreduce the size.

The optical image capturing system 10 of the first embodiment furthersatisfies HVT61=3.3498 mm; HVT62=3.9860 mm; and HVT61/HVT62=0.8404,where HVT61 is a distance perpendicular to the optical axis between thecritical point on the object-side surface 162 of the sixth lens and theoptical axis; and HVT62 is a distance perpendicular to the optical axisbetween the critical point on the image-side surface 166 of the sixthlens and the optical axis.

The optical image capturing system 10 of the first embodiment furthersatisfies InRS71=−0.2756 mm; InRS72=−0.0938 mm; and |InRS72|/TP7=0.0839,where InRS71 is a displacement from a point on the object-side surface172 of the seventh lens 170 passed through by the optical axis to apoint on the optical axis where a projection of the maximum effectivesemi diameter of the object-side surface 172 of the seventh lens 170ends; InRS72 is a displacement from a point on the image-side surface174 of the seventh lens 170 passed through by the optical axis to apoint on the optical axis where a projection of the maximum effectivesemi diameter of the image-side surface 174 of the seventh lens 170ends; and TP7 is a central thickness of the seventh lens 170 on theoptical axis. It is helpful for manufacturing and shaping of the lensesand is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment satisfiesHVT71=3.6822 mm; HVT72=4.0606 mm; and HVT71/HVT72=0.9068, where HVT71 adistance perpendicular to the optical axis between the critical point onthe object-side surface 172 of the seventh lens and the optical axis;and HVT72 a distance perpendicular to the optical axis between thecritical point on the image-side surface 174 of the seventh lens and theoptical axis.

The optical image capturing system 10 of the first embodiment satisfiesHVT72/HOI=0.5414. It is helpful for correction of the aberration of theperipheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfiesHVT72/HOS=0.1505. It is helpful for correction of the aberration of theperipheral view field of the optical image capturing system.

The second lens 120, the third lens 130, and the seventh lens 170 havenegative refractive power. The optical image capturing system 10 of thefirst embodiment further satisfies 1≤NA7/NA2, where NA2 is an Abbenumber of the second lens 120; NA3 is an Abbe number of the third lens130; and NA7 is an Abbe number of the seventh lens 170. It may correctthe aberration of the optical image capturing system.

The optical image capturing system 10 of the first embodiment furthersatisfies |TDT|=2.5678%; |ODT|=2.1302%, where TDT is TV distortion; andODT is optical distortion.

In the present embodiment, the lights of any field of view can befurther divided into sagittal ray and tangential ray, and the spatialfrequency of 220 cycles/mm serves as the benchmark for assessing thefocus shifts and the values of MTF. The focus shifts where thethrough-focus MTF values of the visible sagittal ray at the centralfield of view, 0.3 field of view, and 0.7 field of view of the opticalimage capturing system are at their respective maxima are denoted byVSFS0, VSFS3, and VSFS7 (unit of measurement: mm), respectively. Thevalues of VSFS0, VSFS3, and VSFS7 equal to 0.000 mm, −0.005 mm, and0.000 mm, respectively. The maximum values of the through-focus MTF ofthe visible sagittal ray at the central field of view, 0.3 field ofview, and 0.7 field of view are denoted by VSMTF0, VSMTF3, and VSMTF7,respectively. The values of VSMTF0, VSMTF3, and VSMTF7 equal to 0.886,0.885, and 0.863, respectively. The focus shifts where the through-focusMTF values of the visible tangential ray at the central field of view,0.3 field of view, and 0.7 field of view of the optical image capturingsystem are at their respective maxima, are denoted by VTFS0, VTFS3, andVTFS7 (unit of measurement: mm), respectively. The values of VTFS0,VTFS3, and VTFS7 equal to 0.000 mm, 0.001 mm, and −0.005 mm,respectively. The maximum values of the through-focus MTF of the visibletangential ray at the central field of view, 0.3 field of view, and 0.7field of view are denoted by VTMTF0, VTMTF3, and VTMTF7, respectively.The values of VTMTF0, VTMTF3, and VTMTF7 equal to 0.886, 0.868, and0.796, respectively. The average focus shift (position) of both theaforementioned focus shifts of the visible sagittal ray at three fieldsof view and focus shifts of the visible tangential ray at three fieldsof view is denoted by AVFS (unit of measurement: mm), which satisfiesthe absolute value |(VSFS0+VSFS3+VSFS7+VTFS0+VTFS3+VTFS7)/6|=|0.000 mm|.

The focus shifts where the through-focus MTF values of the infraredsagittal ray at the central field of view, 0.3 field of view, and 0.7field of view of the optical image capturing system are at theirrespective maxima, are denoted by ISFS0, ISFS3, and ISFS7 (unit ofmeasurement: mm), respectively. The values of ISFS0, ISFS3, and ISFS7equal to 0.025 mm, 0.020 mm, and 0.020 mm, respectively. The averagefocus shift (position) of the aforementioned focus shifts of theinfrared sagittal ray at three fields of view is denoted by AISFS (unitof measurement: mm). The maximum values of the through-focus MTF of theinfrared sagittal ray at the central field of view, 0.3 field of view,and 0.7 field of view are denoted by ISMTF0, ISMTF3, and ISMTF7,respectively. The values of ISMTF0, ISMTF3, and ISMTF7 equal to 0.787,0.802, and 0.772, respectively. The focus shifts where the through-focusMTF values of the infrared tangential ray at the central field of view,0.3 field of view, and 0.7 field of view of the optical image capturingsystem are at their respective maxima, are denoted by ITFS0, ITFS3, andITFS7 (unit of measurement: mm), respectively. The values of ITFS0,ITFS3, and ITFS7 equal to 0.025, 0.035, and 0.035, respectively. Theaverage focus shift (position) of the aforementioned focus shifts of theinfrared tangential ray at three fields of view is denoted by AITFS(unit of measurement: mm). The maximum values of the through-focus MTFof the infrared tangential ray at the central field of view, 0.3 fieldof view, and 0.7 field of view are denoted by ITMTF0, ITMTF3, andITMTF7, respectively. The values of ITMTF0, ITMTF3, and ITMTF7 equal to0.787, 0.805, and 0.721, respectively. The average focus shift(position) of both of the aforementioned focus shifts of the infraredsagittal ray at the three fields of view and focus shifts of theinfrared tangential ray at the three fields of view is denoted by AIFS(unit of measurement: mm), which equals to the absolute value of|(ISFS0+ISFS3+ISFS7+ITFS0+ITFS3+ITFS7)/6|=|0.02667 mm|.

The focus shift (difference) between the focal points of the visiblelight and the infrared light at their central fields of view (RGB/IR) ofthe entire optical image capturing system (i.e. wavelength of 850 nmversus wavelength of 555 nm, unit of measurement: mm) is denoted by FS(the distance between the first and second image planes on the opticalaxis), which satisfies the absolute value|(VSFS0+VTFS0)/2−(ISFS0+ITFS0)/2|=|0.025 mm|. The difference (focusshift) between the average focus shift of the visible light in the threefields of view and the average focus shift of the infrared light in thethree fields of view (RGB/IR) of the entire optical image capturingsystem is denoted by AFS (i.e. wavelength of 850 nm versus wavelength of555 nm, unit of measurement: mm), for which the absolute value of|AIFS−AVFS|=|0.02667 mm| is satisfied.

In the optical image capturing system 10 of the first embodiment, atransverse aberration at 0.7 field of view in the positive direction ofthe tangential fan after the shortest operation wavelength of visiblelight passing through the edge of the aperture 100 is denoted by PSTA,and is 0.00040 mm; a transverse aberration at 0.7 field of view in thepositive direction of the tangential fan after the longest operationwavelength of visible light passing through the edge of the aperture 100is denoted by PLTA, and is −0.009 mm; a transverse aberration at 0.7field of view in the negative direction of the tangential fan after theshortest operation wavelength of visible light passing through the edgeof the aperture 100 is denoted by NSTA, and is −0.002 mm; a transverseaberration at 0.7 field of view in the negative direction of thetangential fan after the longest operation wavelength of visible lightpassing through the edge of the aperture 100 is denoted by NLTA, and is−0.016 mm; a transverse aberration at 0.7 field of view of the sagittalfan after the shortest operation wavelength of visible light passingthrough the edge of the aperture 100 is denoted by SSTA, and is 0.018mm; a transverse aberration at 0.7 field of view of the sagittal fanafter the longest operation wavelength of visible light passing throughthe edge of the aperture 100 is denoted by SLTA, and is 0.016 mm.

The parameters of the lenses of the first embodiment are listed in Table1 and Table 2.

TABLE 1 f = 4.3019 mm; f/HEP = 1.2; HAF = 59.9968 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object plane infinity 1 1^(st) lens −1079.4999642.276 plastic 1.565 58.00 −14.53 2 8.304149657 4.552 3 2^(nd) lens14.39130913 5.240 plastic 1.650 21.40 24.25 4 130.0869482 0.162 5 3^(rd)lens 8.167310118 0.837 plastic 1.650 21.40 −97.07 6 6.944477468 1.450 7Aperture plane 0.477 8 4^(th) lens 121.5965254 2.002 plastic 1.565 58.009.75 9 −5.755749302 1.515 10 5^(th) lens −86.27705938 4.271 plastic1.565 58.00 7.16 11 −3.942936258 0.050 12 6^(th) lens 4.867364751 0.300plastic 1.650 21.40 −6.52 13 2.220604983 0.211 14 7^(th) lens1.892510651 1.118 plastic 1.650 21.40 8.29 15 2.224128115 1.400 16Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 0.917 18 Imageplane plane Reference wavelength: 555 nm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k  2.500000E+01 −4.711931E−01   1.531617E+00 −1.153034E+01 −2.915013E+00  4.886991E+00 −3.459463E+01 A4   5.236918E−06 −2.117558E−04  7.146736E−05   4.353586E−04   5.793768E−04 −3.756697E−04 −1.292614E−03A6 −3.014384E−08 −1.838670E−06   2.334364E−06   1.400287E−05  2.112652E−04   3.901218E−04 −1.602381E−05 A8 −2.487400E−10  9.605910E−09 −7.479362E−08 −1.688929E−07 −1.344586E−05 −4.925422E−05−8.452359E−06 A10   1.170000E−12 −8.256000E−11   1.701570E−09  3.829807E−08   1.000482E−06   4.139741E−06   7.243999E−07 A12  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00 A14   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00 Surface 9 10 11 12 13 14 15 k−7.549291E+00 −5.000000E+01 −1.740728E+00 −4.709650E+00 −4.509781E+00−3.427137E+00 −3.215123E+00 A4 −5.583548E−03   1.240671E−04  6.467538E−04 −1.872317E−03 −8.967310E−04 −3.189453E−03 −2.815022E−03A6   1.947110E−04 −4.949077E−05 −4.981838E−05 −1.523141E−05−2.688331E−05 −1.058126E−05   1.884580E−05 A8 −1.486947E−05  2.088854E−06   9.129031E−07 −2.169414E−06 −8.324958E−07   1.760103E−06−1.017223E−08 A10 −6.501246E−08 −1.438383E−08   7.108550E−09−2.308304E−08 −6.184250E−09 −4.730294E−08   3.660000E−12 A12  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00 A14   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00

The figures related to the profile curve lengths obtained based on Table1 and Table 2 are listed in the following table:

First embodiment (Reference wavelength: 555 nm) ARE 1/2(HEP) ARE valueARE-1/2(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.792 1.792 −0.00044  99.98%2.276  78.73% 12 1.792 1.806 0.01319 100.74% 2.276  79.33% 21 1.7921.797 0.00437 100.24% 5.240  34.29% 22 1.792 1.792 −0.00032  99.98%5.240  34.20% 31 1.792 1.808 0.01525 100.85% 0.837  216.01% 32 1.7921.819 0.02705 101.51% 0.837  217.42% 41 1.792 1.792 −0.00041  99.98%2.002  89.50% 42 1.792 1.825 0.03287 101.83% 2.002  91.16% 51 1.7921.792 −0.00031  99.98% 4.271  41.96% 52 1.792 1.845 0.05305 102.96%4.271  43.21% 61 1.792 1.818 0.02587 101.44% 0.300  606.10% 62 1.7921.874 0.08157 104.55% 0.300  624.67% 71 1.792 1.898 0.10523 105.87%1.118  169.71% 72 1.792 1.885 0.09273 105.17% 1.118  168.59% ARS EHD ARSvalue ARS-EHD (ARS/EHD) % TP ARS/TP (%) 11 15.095 15.096 0.001 100.01%2.276  663.24% 12 10.315 11.377 1.062 110.29% 2.276  499.86% 21 7.5318.696 1.166 115.48% 5.240  165.96% 22 4.759 4.881 0.122 102.56% 5.240 93.15% 31 3.632 4.013 0.382 110.51% 0.837  479.55% 32 2.815 3.159 0.344112.23% 0.837  377.47% 41 2.967 2.971 0.004 100.13% 2.002  148.38% 423.402 3.828 0.426 112.53% 2.002  191.20% 51 4.519 4.523 0.004 100.10%4.271  105.91% 52 5.016 5.722 0.706 114.08% 4.271  133.99% 61 5.0195.823 0.805 116.04% 0.300 1941.14% 62 5.629 6.605 0.976 117.34% 0.3002201.71% 71 5.634 6.503 0.869 115.43% 1.118  581.54% 72 6.488 7.1520.664 110.24% 1.118  639.59%

The detail parameters of the first embodiment are listed in Table 1, inwhich the unit of the radius of curvature, thickness, and focal lengthare millimeter, and surface 0-10 indicates the surfaces of all elementsin the system in sequence from the object side to the image side. Table2 is the list of coefficients of the aspheric surfaces, in which A1-A20indicate the coefficients of aspheric surfaces from the first order tothe twentieth order of each aspheric surface. The following embodimentshave the similar diagrams and tables, which are the same as those of thefirst embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 ofthe second embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 210, asecond lens 220, an aperture 200, a third lens 230, a fourth lens 240, afifth lens 250, a sixth lens 260, a seventh lens 270, an infrared raysfilter 280, an image plane 290, and an image sensor 292. FIG. 2C shows atransverse aberration diagram at 0.7 field of view of the secondembodiment of the present invention. FIG. 2D is a diagram showing thethrough-focus MTF values of the visible light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the secondembodiment of the present invention. FIG. 2E is a diagram showing thethrough-focus MTF values of the infrared light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the secondembodiment of the present disclosure.

The first lens 210 has negative refractive power and is made of glass.An object-side surface 212 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 214 thereof, whichfaces the image side, is a concave aspheric surface.

The second lens 220 has positive refractive power and is made of glass.An object-side surface 222 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 224 thereof, whichfaces the image side, is a convex aspheric surface.

The third lens 230 has positive refractive power and is made of glass.An object-side surface 232, which faces the object side, is a convexaspheric surface, and an image-side surface 234, which faces the imageside, is a convex aspheric surface. The object-side surface 232 has aninflection point.

The fourth lens 240 has negative refractive power and is made of glass.An object-side surface 242, which faces the object side, is a concaveaspheric surface, and an image-side surface 244, which faces the imageside, is a concave aspheric surface.

The fifth lens 250 has positive refractive power and is made of glass.An object-side surface 252, which faces the object side, is a convexaspheric surface, and an image-side surface 254, which faces the imageside, is a concave aspheric surface. The image-side surface 254 has aninflection point.

The sixth lens 260 has positive refractive power and is made of glass.An object-side surface 262, which faces the object side, is a concaveaspheric surface, and an image-side surface 264, which faces the imageside, is a convex aspheric surface. Whereby, the incident angle of eachview field could be adjusted to improve aberration.

The seventh lens 270 has negative refractive power and is made of glass.An object-side surface 272, which faces the object side, is a convexsurface, and an image-side surface 274, which faces the image side, is aconcave surface. It may help to shorten the back focal length to keepsmall in size. In addition, the object-side surface 272 and theimage-side surface 274 of the seventh lens 270 both have an inflectionpoint, which may reduce an incident angle of the light of an off-axisfield of view and correct the aberration of the off-axis field of view.

The infrared rays filter 280 is made of glass and between the seventhlens 270 and the image plane 290. The infrared rays filter 280 gives nocontribution to the focal length of the system.

The parameters of the lenses of the second embodiment are listed inTable 3 and Table 4.

TABLE 3 f = 3.4327 mm; f/HEP = 1.6; HAF = 100 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 19.6166335 1.158glass 2.001 29.13 −10.774 2 6.721839156 11.781 3 2^(nd) lens−17.27020661 19.386 glass 2.002 19.32 68.873 4 −21.48152365 15.082 5Aperture 1E+18 0.472 6 3^(rd) lens 10.98236675 6.160 glass 1.517 64.2011.392 7 −10.19189014 2.627 8 4^(th) lens −18.77575846 0.733 glass 2.00219.32 −6.869 9 10.88272273 0.277 10 5^(th) lens 9.669827151 3.254 glass1.517 64.20 15.831 11 −46.01833307 0.244 12 6^(th) lens 12.638822273.896 glass 1.731 40.50 9.420 13 −12.99962017 0.127 14 7^(th) lens−18.60672136 2.687 glass 1.821 24.06 −15.658 15 43.0554211 2.324 16Infrared 1E+18 1.400 BK_7 1.517 64.2 rays filter 17 1E+18 0.668 18 Image1E+18 −0.066 plane Reference wavelength: 555 nm; the position ofblocking light: the elective half diameter of the clear aperture of theeleventh surface is 5.200 mm.

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 3 4 6 7 8 k−3.286298E+00 −5.742797E−01 −2.137095E−02   1.961982E−03   1.182412E−02−9.836431E−03   0.000000E+00 A4   0.000000E+00   0.000000E+00−1.081880E−05   1.343369E−05 −1.160078E−04   1.918672E−04 −3.104472E−04A6   0.000000E+00   0.000000E+00 −3.335007E−08   1.302784E−07−1.240242E−05 −1.036921E−05 −2.218569E−06 A8   0.000000E+00  0.000000E+00   2.234052E−09 −8.624401E−10   3.758659E−07  8.571783E−08   5.682569E−07 A10   0.000000E+00   0.000000E+00−1.543543E−12   7.273375E−12 −1.322970E−08 −1.968699E−09 −2.769705E−09A12   0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00 Surface 9 10 11 12 13 14 15k   0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00 A4 −7.856332E−04−7.981293E−04   3.858082E−04   2.579404E−04   1.354636E−03  1.469066E−03   9.380311E−04 A6   1.576070E−05   2.202758E−05−5.793615E−06 −2.566156E−06 −1.456878E−05 −3.820589E−05 −2.972110E−05 A8−3.569113E−08 −1.328514E−07   3.062593E−07   7.508047E−08   4.049443E−08  3.146218E−07   1.600910E−07 A10   6.602437E−09   3.996820E−10−2.446035E−09 −1.200773E−09 −3.324346E−09 −3.893071E−09 −3.976035E−10A12   0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00

An equation of the aspheric surfaces of the second embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the second embodiment based on Table 3 and Table4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.3186 0.0498 0.3013 0.4997 0.2168 0.3644 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.2192 1.4841 0.4859 3.0543 3.43190.0370 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.1564 6.04590.6674 0.7223 HOS InTL HOS/HOI InS/HOS ODT % TDT % 72.2094 67.883012.0349 0.3435 −97.4917 97.4917 HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PSTA PLTANSTA NLTA SSTA SLTA   0.024 mm −0.008 mm   0.001 mm −0.012 mm   0.022 mm−0.013 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 −0.005 mm −0.010 mm −0.005mm −0.005 mm −0.005 mm −0.005 mm VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3VTMTF7 0.422 0.418 0.438 0.422 0.491 0.344 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3ITFS7 −0.005 mm −0.015 mm −0.015 mm −0.005 mm −0.000 mm   0.010 mmISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.485 0.399 0.332 0.485 0.3850.287 FS AIFS AVFS AFS   0.000 mm −0.005 mm −0.006 mm 0.001 mm

The figures related to the profile curve lengths obtained based on Table3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) ARE 1/2(HEP) ARE valueARE-1/2(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.074 1.074 −0.00025  99.98%1.158  92.72% 12 1.074 1.078 0.00379 100.35% 1.158  93.07% 21 1.0741.074 −0.00009  99.99% 19.386   5.54% 22 1.074 1.073 −0.00033  99.97%19.386   5.54% 31 1.074 1.075 0.00092 100.09% 6.160  17.45% 32 1.0741.075 0.00119 100.11% 6.160  17.45% 41 1.074 1.074 −0.00018  99.98%0.733  146.37% 42 1.074 1.075 0.00089 100.08% 0.733  146.52% 51 1.0741.075 0.00134 100.13% 3.254  33.04% 52 1.074 1.073 −0.00069  99.94%3.254  32.98% 61 1.074 1.074 0.00054 100.05% 3.896  27.57% 62 1.0741.074 0.00033 100.03% 3.896  27.57% 71 1.074 1.074 −0.00027  99.98%2.687  39.95% 72 1.074 1.073 −0.00064  99.94% 2.687  39.94% ARS EHD ARSvalue ARS-EHD (ARS/EHD)% TP ARS/TP (%) 11 16.750 17.780 1.02966 106.15%1.158 1535.60% 12 9.357 14.019 4.66187 149.82% 1.158 1210.78% 21 9.55510.102 0.54749 105.73% 19.386  52.11% 22 10.374 10.713 0.33834 103.26%19.386  55.26% 31 5.299 5.413 0.11396 102.15% 6.160  87.86% 32 5.7996.255 0.45621 107.87% 6.160  101.53% 41 4.722 4.782 0.06028 101.28%0.733  652.03% 42 4.667 4.769 0.10236 102.19% 0.733  650.23% 51 4.8995.070 0.17076 103.49% 3.254  155.83% 52 5.200 5.205 0.00496 100.10%3.254  159.97% 61 6.223 6.633 0.40989 106.59% 3.896  170.24% 62 6.0946.126 0.03239 100.53% 3.896  157.24% 71 6.065 6.134 0.06862 101.13%2.687  228.27% 72 6.282 6.319 0.03705 100.59% 2.687  235.15%

The results of the equations of the second embodiment based on Table 3and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment(Reference wavelength: 555 nm) HIF311 4.0301 HIF311/HOI 0.6717 SGI3110.6940 |SGI311|/(|SGI311| + TP3) 0.1012 HIF521 2.2903 HIF521/HOI 0.3817SGI521 −0.0470 |SGI521|/(|SGI521| + TP5) 0.0142

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system ofthe third embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 310, a secondlens 320, an aperture 300, a third lens 330, a fourth lens 340, a fifthlens 350, a sixth lens 360, a seventh lens 370, an infrared rays filter380, an image plane 390, and an image sensor 392. FIG. 3C shows atransverse aberration diagram at 0.7 field of view of the thirdembodiment of the present invention. FIG. 3D is a diagram showing thethrough-focus MTF values of the visible light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the thirdembodiment of the present invention. FIG. 3E is a diagram showing thethrough-focus MTF values of the infrared light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the thirdembodiment of the present disclosure.

The first lens 310 has negative refractive power and is made of glass.An object-side surface 312 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 314 thereof, whichfaces the image side, is a concave aspheric surface.

The second lens 320 has positive refractive power and is made of glass.An object-side surface 322 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 324 thereof, whichfaces the image side, is a convex aspheric surface.

The third lens 330 has positive refractive power and is made of glass.An object-side surface 332 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 334 thereof, whichfaces the image side, is a convex aspheric surface. The object-sidesurface 322 has an inflection point.

The fourth lens 340 has negative refractive power and is made of glass.An object-side surface 342, which faces the object side, is a concaveaspheric surface, and an image-side surface 344, which faces the imageside, is a concave aspheric surface. The image-side surface 344 has aninflection point.

The fifth lens 350 has positive refractive power and is made of glass.An object-side surface 352, which faces the object side, is a concaveaspheric surface, and an image-side surface 354, which faces the imageside, is a convex aspheric surface. The object-side surface 352 has aninflection point. It may help to shorten the back focal length to keepsmall in size.

The sixth lens 360 has positive refractive power and is made of glass.An object-side surface 362, which faces the object side, is a concaveaspheric surface, and an image-side surface 364, which faces the imageside, is a convex aspheric surface. The image-side surface 364 has twoinflection points. Whereby, the incident angle of each view field couldbe adjusted to improve aberration.

The seventh lens 370 has negative refractive power and is made of glass.An object-side surface 372, which faces the object side, is a convexaspheric surface, and an image-side surface 374, which faces the imageside, is a concave aspheric surface. It may help to shorten the backfocal length to keep small in size. In addition, the object-side surface372 has two inflection points, which may reduce an incident angle of thelight of an off-axis field of view and correct the aberration of theoff-axis field of view.

The infrared rays filter 380 is made of glass and between the seventhlens 370 and the image plane 390. The infrared rays filter 380 gives nocontribution to the focal length of the system.

The parameters of the lenses of the third embodiment are listed in Table5 and Table 6.

TABLE 5 f = 4.6650 mm; f/HEP = 1.6; HAF = 100 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 31.87773608 0.734glass 2.001 29.13 −10.066 2 7.525338636 7.030 3 2^(nd) lens −14.0192864515.480 glass 2.002 19.32 22.569 4 −13.35236717 5.668 5 Aperture 1E+182.398 6 3^(rd) lens 33.83858873 4.776 glass 1.517 64.20 13.062 7−7.992652506 0.229 8 4^(th) lens −24.75687104 2.554 glass 2.002 19.32−8.511 9 13.44578513 0.401 10 5^(th) lens 19.01331691 2.765 glass 1.51764.20 18.299 11 −17.75918235 6.469 12 6^(th) lens 10.90509822 5.107glass 1.731 40.50 13.918 13 −112.1544402 1.316 14 7^(th) lens−14.96225569 2.587 glass 1.821 24.06 −72.433 15 −21.60690687 1.297 16Infrared 1E+18 1.400 BK_7 1.517 64.2 rays filter 17 1E+18 0.666 18 Image1E+18 −0.066 plane Reference wavelength: 555 nm; the position ofblocking light: the effective half diameter of the clear aperture of thetenth surface is 5.00 mm.

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 3 4 6 7 8 k3.038473E+00 3.263032E−01 1.730655E+00 4.464327E−02 −4.389530E+01−3.024805E−01 0.000000E+00 A4 0.000000E+00 0.000000E+00 5.910836E−055.202189E−05 −5.020100E−05  6.248803E−04 1.539911E−04 A6 0.000000E+000.000000E+00 −5.592292E−07  1.346320E−07 −1.026106E−05 −1.014509E−05−6.796946E−06  A8 0.000000E+00 0.000000E+00 3.401277E−08 9.770012E−10 6.166745E−07 −1.517314E−07 −1.946787E−07  A10 0.000000E+00 0.000000E+000.000000E+00 −8.329091E−12  −1.855564E−08  0.000000E+00 0.000000E+00 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k  0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A4 −2.201098E−04 −9.938403E−05 −7.126291E−05 1.038270E−042.445197E−04 1.275777E−03 2.045753E−03 A6 −4.711901E−06 −8.412099E−07−2.093408E−07 −3.648193E−07  6.377880E−07 −3.578605E−05  −4.615934E−05 A8 −1.119655E−08 −1.490267E−07 −1.439215E−07 8.142455E−09 −3.799621E−08 4.108349E−07 2.427116E−07 A10  0.000000E+00  0.000000E+00  0.000000E+000.000000E+00 0.000000E+00 −1.879549E−09  8.708230E−10 A12  0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00

An equation of the aspheric surfaces of the third embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the third embodiment based on Table 5 and Table6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.4635 0.2067 0.3571 0.5481 0.2549 0.3352 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.0644 1.7039 0.5260 3.2391 1.50700.2821 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.4460 1.72780.5015 0.7642 HOS InTL HOS/HOI InS/HOS ODT % TDT % 60.8093 57.512010.1349 0.5245 −122.5920 96.1099 HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PSTA PLTANSTA NLTA SSTA SLTA −0.054 mm −0.019 mm −0.004 mm   0.004 mm −0.056 mm−0.025 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 −0.000 mm −0.010 mm −0.010mm −0.000 mm   0.005 mm   0.010 mm VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3VTMTF7 0.536 0.505 0.550 0.536 0.511 0.234 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3ITFS7   0.008 mm −0.000 mm   0.005 mm   0.010 mm   0.020 mm   0.035 mmISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.557 0.529 0.519 0.557 0.5650.320 FS AIFS AVFS AFS   0.008 mm   0.013 mm −0.001 mm 0.014 mm

The figures related to the profile curve lengths obtained based on Table5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE− ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.464 1.465 0.00031 100.02% 0.734199.62% 12 1.464 1.473 0.00926 100.63% 0.734 200.84% 21 1.464 1.4670.00248 100.17% 15.480 9.47% 22 1.464 1.467 0.00273 100.19% 15.480 9.48%31 1.464 1.464 0.00022 100.02% 4.776 30.66% 32 1.464 1.472 0.00766100.52% 4.776 30.82% 41 1.464 1.465 0.00062 100.04% 2.554 57.36% 421.464 1.467 0.00261 100.18% 2.554 57.44% 51 1.464 1.465 0.00122 100.08%2.765 53.00% 52 1.464 1.466 0.00148 100.10% 2.765 53.01% 61 1.464 1.4680.00428 100.29% 5.107 28.76% 62 1.464 1.464 −0.00017 99.99% 5.107 28.67%71 1.464 1.466 0.00174 100.12% 2.587 56.68% 72 1.464 1.465 0.00050100.03% 2.587 56.63% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP(%) 11 11.564 11.938 0.37401 103.23% 0.734 1627.22% 12 6.501 9.0182.51666 138.71% 0.734 1229.17% 21 6.376 6.641 0.26473 104.15% 15.48042.90% 22 7.928 8.381 0.45346 105.72% 15.480 54.14% 31 4.945 4.9500.00485 100.10% 4.776 103.64% 32 5.189 5.531 0.34186 106.59% 4.776115.81% 41 4.753 4.793 0.04021 100.85% 2.554 187.69% 42 4.989 5.0570.06734 101.35% 2.554 198.02% 51 5.000 5.035 0.03499 100.70% 2.765182.11% 52 5.347 5.479 0.13180 102.46% 2.765 198.18% 61 7.566 8.5731.00707 113.31% 5.107 167.88% 62 6.938 6.947 0.00922 100.13% 5.107136.04% 71 6.886 6.986 0.10026 101.46% 2.587 270.10% 72 6.711 6.7250.01402 100.21% 2.587 259.98%

The results of the equations of the third embodiment based on Table 5and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment(Reference wavelength: 555 nm) HIF311 3.1357 HIF311/HOI 0.5226 SGI3110.1234 |SGI311|/(|SGI311| + TP3) 0.0252 HIF421 4.0790 HIF421/HOI 0.6798SGI421 0.5502 |SGI421|/(|SGI421| + TP4) 0.1773 HIF511 3.9459 HIF511/HOI0.6577 SGI511 0.3779 |SGI511|/(|SGI511| + TP5) 0.1203 HIF621 1.7320HIF621/HOI 0.2887 SGI621 −0.0112 |SGI621|/(|SGI621| + TP6) 0.0022 HIF6226.3629 HIF622/HOI 1.0605 SGI622 0.1604 |SGI622|/(|SGI622| + TP6) 0.0305HIF711 1.4681 HIF711/HOI 0.2447 SGI711 −0.0409 |SGI711|/(|SGI711| + TP7)0.0156 HIF721 4.5513 HIF721/HOI 0.7585 SGI721 0.0307|SGI721|/(|SGI721| + TP7) 0.0117

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 ofthe fourth embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 410, asecond lens 420, a third lens 430, an aperture 400, a fourth lens 440, afifth lens 450, a sixth lens 460, a seventh lens 470, an infrared raysfilter 480, an image plane 490, and an image sensor 492. FIG. 4C shows aa transverse aberration diagram at 0.7 field of view of the fourthembodiment of the present invention. FIG. 4D is a diagram showing thethrough-focus MTF values of the visible light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the fourthembodiment of the present invention. FIG. 4E is a diagram showing thethrough-focus MTF values of the infrared light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the fourthembodiment of the present disclosure.

The first lens 410 has negative refractive power and is made of glass.An object-side surface 412 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 414 thereof, whichfaces the image side, is a concave aspheric surface.

The second lens 420 has negative refractive power and is made of glass.An object-side surface 422 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 424 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 422 has three inflection points.

The third lens 430 has positive refractive power and is made of glass.An object-side surface 432 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 434 thereof, whichfaces the image side, is a convex aspheric surface.

The fourth lens 440 has positive refractive power and is made of glass.An object-side surface 442, which faces the object side, is a convexaspheric surface, and an image-side surface 444, which faces the imageside, is a convex aspheric surface.

The fifth lens 450 has positive refractive power and is made of glass.An object-side surface 452, which faces the object side, is a convexaspheric surface, and an image-side surface 454, which faces the imageside, is a convex aspheric surface.

The sixth lens 460 has negative refractive power and is made of glass.An object-side surface 462, which faces the object side, is a convexaspheric surface, and an image-side surface 464, which faces the imageside, is a concave aspheric surface. Whereby, the incident angle of eachview field could be adjusted to improve aberration.

The seventh lens 470 has positive refractive power and is made of glass.An object-side surface 472, which faces the object side, is a convexaspheric surface, and an image-side surface 474, which faces the imageside, is a convex aspheric surface. It may help to shorten the backfocal length to keep small in size. In addition, it may reduce anincident angle of the light of an off-axis field of view and correct theaberration of the off-axis field of view.

The infrared rays filter 480 is made of glass and between the seventhlens 470 and the image plane 490. The infrared rays filter 480 gives nocontribution to the focal length of the system.

The parameters of the lenses of the fourth embodiment are listed inTable 7 and Table 8.

TABLE 7 f = 3.3691 mm; f/HEP = 1.6; HAF = 100 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 18.53465975 1.732glass 2.001 29.13 −14.872 2 7.895641835 9.378 3 2^(nd) lens −68.465069751.463 glass 1.702 41.15 −10.300 4 8.190388033 2.487 5 3^(rd) lens27.54936977 18.545 glass 2.002 19.32 21.363 6 −66.13224074 6.603 7Aperture 1E+18 0.200 8 4^(th) lens 20.68817509 2.478 glass 1.497 81.5614.659 9 −10.83858406 0.218 10 5^(th) lens 8.984929816 4.354 glass 1.49781.56 12.939 11 −19.13849739 0.531 12 6^(th) lens 41.4887939 1.565 glass2.002 19.32 −7.874 13 6.552024662 1.421 14 7^(th) lens 27.43112034 6.412glass 1.487 70.44 16.746 15 −10.77055437 0.611 16 Infrared 1E+18 1.000BK_7 1.517 64.2 rays filter 17 1E+18 1.000 18 Image 1E+18 0.000 planeReference wavelength: 555 nm; the position of blocking light: none.

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k−2.415516E+00  −2.043627E−01  0.000000E+00  0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A4 5.005216E−06 −2.497868E−05  1.163338E−04−1.029252E−04 −2.878851E−05  2.259564E−05 8.050329E−05 A6 0.000000E+000.000000E+00 −1.135504E−06  −1.622858E−07 −1.941732E−07  −3.396594E−07 −4.924829E−06  A8 0.000000E+00 0.000000E+00 1.971134E−09 −7.896455E−080.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+002.648258E−11  6.247517E−10 0.000000E+00 0.000000E+00 0.000000E+00 A120.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 2.544076E−04 −2.800232E−04  −2.016346E−04 −1.080235E−04  −2.343676E−04  −4.070383E−05   9.879287E−04 A6−1.776479E−06  −3.721655E−06  3.581189E−07 1.665651E−06 3.183615E−062.258674E−05 −8.401761E−06 A8 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 −1.468302E−06  −1.215394E−07 A10 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 3.936620E−08−3.464589E−10 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00  0.000000E+00

An equation of the aspheric surfaces of the fourth embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the fourth embodiment based on Table 7 and Table8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.2265 0.3271 0.1577 0.2298 0.2604 0.4279 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.2012 1.0420 0.7887 1.3212 2.78350.4218 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.4439 0.48227.5921 5.0049 HOS InTL HOS/HOI InS/HOS ODT % TDT % 59.9994 57.38879.9999 0.3298 −131.4420 95.8425 HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PSTA PLTANSTA NLTA SSTA SLTA 0.022 mm −0.004 mm   0.003 mm 0.002 mm   0.008 mm−0.004 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 0.010 mm −0.005 mm −0.000mm 0.010 mm −0.005 mm −0.010 mm VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3VTMTF7 0.708 0.672 0.562 0.708 0.563 0.423 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3ITFS7 0.015 mm −0.005 mm −0.000 mm 0.015 mm −0.005 mm −0.020 mm ISMTF0ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.738 0.725 0.698 0.738 0.726 0.625FS AIFS AVFS AFS 0.005 mm −0.000 mm −0.000 mm 0.000 mm

The figures related to the profile curve lengths obtained based on Table7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 0.991 0.990 −0.00045 99.95%1.732 57.18% 12 0.991 0.993 0.00168 100.17% 1.732 57.30% 21 0.991 0.990−0.00089 99.91% 1.463 67.65% 22 0.991 0.992 0.00149 100.15% 1.463 67.82%31 0.991 0.990 −0.00071 99.93% 18.545 5.34% 32 0.991 0.990 −0.0008999.91% 18.545 5.34% 41 0.991 0.990 −0.00054 99.95% 2.478 39.96% 42 0.9910.991 0.00044 100.04% 2.478 40.00% 51 0.991 0.992 0.00107 100.11% 4.35422.78% 52 0.991 0.990 −0.00047 99.95% 4.354 22.75% 61 0.991 0.990−0.00083 99.92% 1.565 63.26% 62 0.991 0.994 0.00286 100.29% 1.565 63.50%71 0.991 0.990 −0.00071 99.93% 6.412 15.44% 72 0.991 0.991 0.00041100.04% 6.412 15.46% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP(%) 11 16.296 17.704 1.40786 108.64% 1.732 1022.00% 12 8.775 13.3304.55504 151.91% 1.732 769.52% 21 8.291 8.295 0.00337 100.04% 1.463566.81% 22 6.631 7.465 0.83345 112.57% 1.463 510.09% 31 6.651 6.7030.05233 100.79% 18.545 36.14% 32 5.556 5.562 0.00557 100.10% 18.54529.99% 41 4.524 4.559 0.03462 100.77% 2.478 183.94% 42 4.748 4.8790.13114 102.76% 2.478 196.87% 51 5.164 5.386 0.22199 104.30% 4.354123.70% 52 5.052 5.141 0.08925 101.77% 4.354 118.08% 61 4.606 4.6130.00665 100.14% 1.565 294.75% 62 4.100 4.405 0.30515 107.44% 1.565281.48% 71 4.317 4.340 0.02366 100.55% 6.412 67.70% 72 5.489 5.5850.09612 101.75% 6.412 87.10%

The results of the equations of the fourth embodiment based on Table 7and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment(Reference wavelength: 555 nm) HIF211 4.1416 HIF211/HOI 0.6903 SGI211−0.0967 |SGI211|/(|SGI211| + TP2) 0.0620 HIF212 6.2052 HIF212/HOI 1.0342SGI212 −0.1676 |SGI212|/(|SGI212| + TP2) 0.1027 HIF213 7.6155 HIF213/HOI1.2692 SGI213 −0.2154 |SGI213|/(|SGI213| + TP2) 0.1283

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system ofthe fifth embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 510, a secondlens 520, a third lens 530, an aperture 500, a fourth lens 540, a fifthlens 550, a sixth lens 560, a seventh lens 570, an infrared rays filter580, an image plane 590, and an image sensor 592. FIG. 5C shows atransverse aberration diagram at 0.7 field of view of the fifthembodiment of the present invention. FIG. 5D is a diagram showing thethrough-focus MTF values of the visible light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the fifthembodiment of the present invention. FIG. 5E is a diagram showing thethrough-focus MTF values of the infrared light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the fifthembodiment of the present disclosure.

The first lens 510 has negative refractive power and is made of glass.An object-side surface 512, which faces the object side, is a convexaspheric surface, and an image-side surface 514, which faces the imageside, is a concave aspheric surface.

The second lens 520 has negative refractive power and is made of glass.An object-side surface 522 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 524 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 522 has an inflection point.

The third lens 530 has positive refractive power and is made of glass.An object-side surface 532, which faces the object side, is a convexaspheric surface, and an image-side surface 534, which faces the imageside, is a convex aspheric surface. The object-side surface 532 has aninflection point.

The fourth lens 540 has positive refractive power and is made of glass.An object-side surface 542, which faces the object side, is a convexaspheric surface, and an image-side surface 544, which faces the imageside, is a convex aspheric surface. The object-side surface 542 has aninflection point.

The fifth lens 550 has positive refractive power and is made of glass.An object-side surface 552, which faces the object side, is a convexaspheric surface, and an image-side surface 554, which faces the imageside, is a convex aspheric surface.

The sixth lens 560 has negative refractive power and is made of glass.An object-side surface 562, which faces the object side, is a concaveaspheric surface, and an image-side surface 564, which faces the imageside, is a concave aspheric surface. The object-side surface 562 has aninflection point. Whereby, the incident angle of each view field couldbe adjusted to improve aberration.

The seventh lens 570 has positive refractive power and is made of glass.An object-side surface 572, which faces the object side, is a convexsurface, and an image-side surface 574, which faces the image side, is aconcave surface. The object-side surface 572 and the image-side surface574 both have an inflection point. It may help to shorten the back focallength to keep small in size. In addition, it may reduce an incidentangle of the light of an off-axis field of view and correct theaberration of the off-axis field of view.

The infrared rays filter 570 is made of glass and between the seventhlens 570 and the image plane 590. The infrared rays filter 570 gives nocontribution to the focal length of the system.

The parameters of the lenses of the fifth embodiment are listed in Table9 and Table 10.

TABLE 9 f = 3.6938 mm; f/HEP = 1.6; HAF = 100 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 26.04752593 0.800glass 2.001 29.13 −14.887 2 9.36942059 11.132 3 2^(nd) lens −24.075383260.800 glass 1.702 41.15 −12.551 4 14.17078456 2.918 5 3^(rd) lens48067.86686 10.874 glass 2.002 19.32 19.831 6 −20.05419554 11.836 7Aperture 1E+18 0.200 8 4^(th) lens 128.1427365 2.357 glass 1.497 81.5625.011 9 −13.7186201 0.200 10 5^(th) lens 10.05654735 3.919 glass 1.49781.56 11.916 11 −12.61469465 0.200 12 6^(th) lens −14.92455429 6.785glass 2.002 19.32 −11.532 13 65.44491518 2.195 14 7^(th) lens9.151216693 4.509 glass 1.487 70.44 36.652 15 15.68184913 1.274 16Infrared 1E+18 1.000 BK_7 1.517 64.2 rays filter 17 1E+18 1.009 18 Image1E+18 −0.010 plane Reference wavelength: 555 nm; the position ofblocking light: none

TABLE 10 Coefficients of the aspheric surfaces Sur- face 1 2 3 4 5 6 8 k4.977522E−01 5.230785E−03 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A4 −7.818697E−06 1.355186E−05 −1.100280E−051.945605E−05 −1.993607E−05 6.352256E−06 5.514564E−05 A6 0.000000E+000.000000E+00 1.251689E−07 −6.684149E−07 −8.120822E−07 −2.483224E−07−1.081438E−05 A8 0.000000E+00 0.000000E+00 3.903884E−09 4.244273E−090.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00−1.957948E−11 2.623831E−10 0.000000E+00 0.000000E+00 0.000000E+00 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 Sur- face 9 10 11 12 13 14 15 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A4 −1.053793E−04 −3.465284E−04 −1.271129E−04 1.966834E−041.246335E−04 −2.473171E−04 8.439771E−05 A6 −2.542850E−06 −4.489230E−071.605971E−06 8.811723E−07 −2.133064E−08 −1.847262E−06 5.573526E−07 A80.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−1.795922E−08 −4.789740E−08 A10 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 −1.782672E−09 −2.773460E−09 A12 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00

An equation of the aspheric surfaces of the fifth embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the fifth embodiment based on Table 9 and Table10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.2481 0.2943 0.1863 0.1477 0.3100 0.3203 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.1008 0.9024 0.7051 1.2799 3.01370.5943 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.1861 0.632914.9146 0.9880 HOS InTL HOS/HOI InS/HOS ODT % TDT % 61.9995 58.725710.3333 0.3813 −128.6440 89.4276 HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.5069 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PSTA PLTANSTA NLTA SSTA SLTA   0.012 mm   0.006 mm   0.003 mm   0.004 mm   0.005mm −0.007 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 −0.000 mm −0.005 mm−0.000 mm −0.000 mm −0.000 mm −0.005 mm VSMTF0 VSMTF3 VSMTF7 VTMTF0VTMTF3 VTMTF7 0.668 0.673 0.669 0.668 0.677 0.556 ISFS0 ISFS3 ISFS7ITFS0 ITFS3 ITFS7 −0.000 mm −0.005 mm −0.000 mm −0.000 mm −0.000 mm−0.000 mm ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.774 0.784 0.7740.774 0.786 0.715 FS AIFS AVFS AFS   0.000 mm −0.001 mm −0.002 mm 0.001mm

The figures related to the profile curve lengths obtained based on Table9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE− ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.154 1.154 0.00008 100.01% 0.800144.30% 12 1.154 1.157 0.00264 100.23% 0.800 144.62% 21 1.154 1.1540.00015 100.01% 0.800 144.31% 22 1.154 1.155 0.00099 100.09% 0.800144.41% 31 1.154 1.154 −0.00030 99.97% 10.874 10.61% 32 1.154 1.1550.00034 100.03% 10.874 10.62% 41 1.154 1.154 −0.00028 99.98% 2.35748.97% 42 1.154 1.155 0.00108 100.09% 2.357 49.03% 51 1.154 1.1560.00220 100.19% 3.919 29.51% 52 1.154 1.156 0.00134 100.12% 3.919 29.49%61 1.154 1.155 0.00084 100.07% 6.785 17.02% 62 1.154 1.154 −0.0002399.98% 6.785 17.01% 71 1.154 1.157 0.00274 100.24% 4.509 25.66% 72 1.1541.155 0.00076 100.07% 4.509 25.62% ARS EHD ARS value ARS − EHD(ARS/EHD)% TP ARS/TP (%) 11 17.512 19.233 1.72100 109.83% 0.800 2404.07%12 9.343 14.506 5.16320 155.26% 0.800 1813.25% 21 9.018 9.212 0.19395102.15% 0.800 1151.44% 22 7.686 8.212 0.52564 106.84% 0.800 1026.45% 317.715 7.726 0.01066 100.14% 10.874 71.05% 32 9.014 9.385 0.37157 104.12%10.874 86.31% 41 4.674 4.674 0.00045 100.01% 2.357 198.34% 42 5.0525.210 0.15747 103.12% 2.357 221.08% 51 5.736 5.945 0.20978 103.66% 3.919151.70% 52 5.754 6.004 0.24933 104.33% 3.919 153.18% 61 5.529 5.6090.07978 101.44% 6.785 82.66% 62 5.464 5.480 0.01616 100.30% 6.785 80.77%71 6.011 6.299 0.28856 104.80% 4.509 139.70% 72 5.955 6.077 0.12210102.05% 4.509 134.78%

The results of the equations of the fifth embodiment based on Table 9and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment(Reference wavelength: 555 nm) HIF211 8.8636 HIF211/HOI 1.4773 SGI211−1.6081 |SGI211|/(|SGI211| + TP2) 0.6678 HIF311 0.2936 HIF311/HOI 0.0489SGI311 0.000001 |SGI311|/(|SGI311| + TP3) 0.0000 HIF411 2.4556HIF411/HOI 0.4093 SGI411 0.0232 |SGI411|/(|SGI411| + TP4) 0.0097 HIF6115.1454 HIF611/HOI 0.8576 SGI611 −0.7608 |SGI611|/(|SGI611| + TP6) 0.1008HIF711 4.9907 HIF711/HOI 0.8318 SGI711 1.2747 |SGI711|/(|SGI711| + TP7)0.2204 HIF721 4.8215 HIF721/HOI 0.8036 SGI721 0.7794|SGI721|/(|SGI721| + TP7) 0.1474

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system ofthe sixth embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 610, a secondlens 620, a third lens 630, an aperture 600, a fourth lens 640, a fifthlens 650, a sixth lens 660, a seventh lens 670, an infrared rays filter680, an image plane 690, and an image sensor 692. FIG. 6C shows atransverse aberration diagram at 0.7 field of view of the sixthembodiment of the present invention. FIG. 6D is a diagram showing thethrough-focus MTF values of the visible light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the sixthembodiment of the present invention. FIG. 6E is a diagram showing thethrough-focus MTF values of the infrared light spectrum at the centralfield of view, 0.3 field of view, and 0.7 field of view of the sixthembodiment of the present disclosure.

The first lens 610 has negative refractive power and is made of glass.An object-side surface 612, which faces the object side, is a convexaspheric surface, and an image-side surface 614, which faces the imageside, is a concave aspheric surface.

The second lens 620 has negative refractive power and is made of glass.An object-side surface 622 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 624 thereof, whichfaces the image side, is a concave aspheric surface.

The third lens 630 has positive refractive power and is made of glass.An object-side surface 632, which faces the object side, is a convexaspheric surface, and an image-side surface 634, which faces the imageside, is a convex aspheric surface. The object-side surface 632 has aninflection point.

The fourth lens 640 has positive refractive power and is made of glass.An object-side surface 642, which faces the object side, is a convexspherical surface, and an image-side surface 644, which faces the imageside, is a convex spherical surface. The object-side surface 642 has aninflection point.

The fifth lens 650 has positive refractive power and is made of glass.An object-side surface 652, which faces the object side, is a convexaspheric surface, and an image-side surface 654, which faces the imageside, is a convex aspheric surface. The object-side surface 652 has aninflection point.

The sixth lens 660 has negative refractive power and is made of glass.An object-side surface 662, which faces the object side, is a convexsurface, and an image-side surface 664, which faces the image side, is aconcave surface. The object-side surface 662 has an inflection point,and the image-side surface 664 has two inflection points. Whereby, theincident angle of each view field could be adjusted to improveaberration.

The seventh lens 670 has positive refractive power and is made of glass.An object-side surface 672, which faces the object side, is a convexsurface, and an image-side surface 674, which faces the image side, is aconcave surface. The object-side surface 672 and the image-side surface674 both have an inflection point. It may help to shorten the back focallength to keep small in size. In addition, it may reduce an incidentangle of the light of an off-axis field of view and correct theaberration of the off-axis field of view.

The infrared rays filter 680 is made of glass and between the seventhlens 670 and the image plane 690. The infrared rays filter 680 gives nocontribution to the focal length of the system.

The parameters of the lenses of the sixth embodiment are listed in Table11 and Table 12.

TABLE 11 f = 3.5464 mm; f/HEP = 1.6; HAF = 100 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 22.88430929 0.984glass 2.001 29.13 −14.370 2 8.674788468 9.959 3 2^(nd) lens −38.488916230.877 glass 1.702 41.15 −11.106 4 9.914991596 2.551 5 3^(rd) lens59.83784628 16.146 glass 2.002 19.32 20.211 6 −26.81847543 5.302 7Aperture 1E+18 0.200 8 4^(th) lens 26.15933327 2.538 glass 1.497 81.5617.658 9 −12.8276443 0.213 10 5^(th) lens 10.42549518 3.825 glass 1.49781.56 13.658 11 −17.20317991 0.249 12 6^(th) lens 160.2867233 0.852glass 2.002 19.32 −9.138 13 8.711865252 2.333 14 7^(th) lens 9.3464540997.952 glass 1.487 70.44 21.885 15 53.36494381 0.777 16 Infrared 1E+181.000 BK_7 1.517 64.2 rays filter 17 1E+18 1.009 18 Image 1E+18 −0.010plane Reference wavelength: 555 nm; the position of blocking light:none.

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k−4.162347E−01  −1.621617E−01   0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A4 3.567992E−06 −1.060193E−05  −2.509887E−051.399794E−04 4.797559E−05 6.503323E−05 1.833803E−04 A6 0.000000E+000.000000E+00 −6.119929E−07 2.322027E−07 −1.803934E−06  −6.074623E−07 −5.433956E−06  A8 0.000000E+00 0.000000E+00  3.698215E−08 −1.343334E−07 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00−3.062447E−10 3.505012E−09 0.000000E+00 0.000000E+00 0.000000E+00 A120.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A4 1.535885E−04 −2.831492E−04  −1.526129E−04 −2.322772E−04  −2.562242E−04  1.575578E−05 3.368237E−04 A6−1.023699E−06  −2.020471E−06  −6.606161E−07  2.488900E−06 −1.478217E−06 −8.660583E−06  5.143847E−06 A8 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 2.049024E−07 4.329106E−08 A10 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −4.410967E−09 −8.440398E−09  A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the sixth embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the sixth embodiment based on Table 11 and Table12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.2468 0.3193 0.1755 0.2008 0.2597 0.3881 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.1620 1.2708 0.4814 2.6400 2.80820.6578 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.2939 0.549512.4809 12.0720 HOS InTL HOS/HOI InS/HOS ODT % TDT % 56.7579 53.98149.4597 0.3689 −130.7540 97.8054 HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 2.7674 0.0000 0.0000 5.8424 0.9737 0.1029 PSTA PLTANSTA NLTA SSTA SLTA −0.005 mm   0.00021 mm −0.003 mm   0.010 mm   0.009mm −0.00041 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 −0.005 mm  −0.005 mm  0.005 mm −0.005 mm −0.000 mm  −0.000 mm VSMTF0 VSMTF3 VSMTF7 VTMTF0VTMTF3 VTMTF7   0.689 0.654 0.638 0.689 0.640 0.481 ISFS0 ISFS3 ISFS7ITFS0 ITFS3 ITFS7 −0.000 mm  −0.000 mm   0.005 mm −0.000 mm   0.005 mm   0.015 mm ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.786 0.697 0.5390.786 0.635 0.399 FS AIFS AVFS AFS   0.005 mm    0.004 mm −0.002 mm0.006 mm

The figures related to the profile curve lengths obtained based on Table11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE− ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.108 1.108 0.00018 100.02% 0.984112.69% 12 1.108 1.111 0.00277 100.25% 0.984 112.95% 21 1.108 1.108−0.00010 99.99% 0.877 126.39% 22 1.108 1.110 0.00208 100.19% 0.877126.64% 31 1.108 1.108 −0.00019 99.98% 16.146 6.86% 32 1.108 1.1080.00005 100.00% 16.146 6.86% 41 1.108 1.108 0.00008 100.01% 2.538 43.68%42 1.108 1.109 0.00111 100.10% 2.538 43.72% 51 1.108 1.110 0.00180100.16% 3.825 29.02% 52 1.108 1.109 0.00052 100.05% 3.825 28.99% 611.108 1.108 −0.00025 99.98% 0.852 130.05% 62 1.108 1.111 0.00271 100.24%0.852 130.40% 71 1.108 1.111 0.00235 100.21% 7.952 13.97% 72 1.108 1.108−0.00017 99.98% 7.952 13.93% ARS EHD ARS value ARS − EHD (ARS/EHD)% TPARS/TP (%) 11 15.855 17.390 1.53530 109.68% 0.984 1767.92% 12 9.24813.237 3.98955 143.14% 0.984 1345.75% 21 7.749 7.797 0.04800 100.62%0.877 889.31% 22 6.269 6.919 0.65003 110.37% 0.877 789.22% 31 6.3006.309 0.00855 100.14% 16.146 39.07% 32 6.560 6.614 0.05372 100.82%16.146 40.96% 41 5.207 5.245 0.03801 100.73% 2.538 206.69% 42 5.2735.404 0.13111 102.49% 2.538 212.96% 51 5.674 5.860 0.18586 103.28% 3.825153.18% 52 5.642 5.799 0.15761 102.79% 3.825 151.61% 61 5.229 5.2290.00002 100.00% 0.852 613.72% 62 4.945 5.182 0.23744 104.80% 0.852608.27% 71 5.858 6.202 0.34471 105.88% 7.952 78.00% 72 6.082 6.1280.04562 100.75% 7.952 77.06%

The results of the equations of the sixth embodiment based on Table 11and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment(Reference wavelength: 555 nm) HIF211 0.6369 HIF211/HOI 0.0849 SGI2110.0079 |SGI211|/(|SGI211| + TP2) 0.0137 HIF311 1.9361 HIF311/HOI 0.2581SGI311 −0.2607 |SGI311|/(|SGI311| + TP3) 0.4017 HIF411 2.3709 HIF411/HOI0.3161 SGI411 −0.3518 |SGI411|/(|SGI411| + TP4) 0.6376 HIF421 1.7502HIF421/HOI 0.2334 SGI421 −0.1043 |SGI421|/(|SGI421| + TP4) 0.3427 HIF5111.5428 HIF511/HOI 0.2057 SGI511 0.1156 |SGI511|/(|SGI511| + TP5) 0.1558HIF521 1.0772 HIF521/HOI 0.1436 SGI521 0.0545 |SGI521|/(|SGI521| + TP5)0.0800 HIF621 2.2109 HIF621/HOI 0.2948 SGI621 −0.7760|SGI621|/(|SGI621| + TP6) 0.3289 HIF622 3.1845 HIF622/HOI 0.4246 SGI622−1.2376 |SGI622|/(|SGI622| + TP6) 0.4387 HIF711 0.6044 HIF711/HOI 0.0806SGI711 0.0048 |SGI711|/(|SGI711| + TP7) 0.0057 HIF721 1.2594 HIF721/HOI0.1679 SGI721 0.2719 |SGI721|/(|SGI721| + TP7) 0.2437

It must be pointed out that the embodiments described above are onlysome embodiments of the present invention. All equivalent structureswhich employ the concepts disclosed in this specification and theappended claims should fall within the scope of the present invention.

What is claimed is:
 1. An optical image capturing system, in order alongan optical axis from an object side to an image side, comprising: afirst lens having refractive power; a second lens having refractivepower; a third lens having refractive power; a fourth lens havingrefractive power; a fifth lens having refractive power; a sixth lenshaving refractive power; a seventh lens having refractive power; a firstimage plane, which is an image plane specifically for visible light andperpendicular to the optical axis; a through-focus modulation transferrate (value of MTF) at a first spatial frequency having a maximum valueat central field of view of the first image plane; and a second imageplane, which is an image plane specifically for infrared light andperpendicular to the optical axis; the through-focus modulation transferrate (value of MTF) at the first spatial frequency having a maximumvalue at central of field of view of the second image plane; wherein theoptical image capturing system consists of the seven lenses withrefractive power; at least one lens among the first lens to the seventhlens has positive refractive power; each lens among the first lens tothe seventh lens has an object-side surface, which faces the objectside, and an image-side surface, which faces the image side; wherein theoptical image capturing system satisfies:1.0≤f/HEP≤10.0;0 deg<HAF≤150 deg; and|FS|≤60 μm; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths ofthe first lens to the seventh lens, respectively; f is a focal length ofthe optical image capturing system; HEP is an entrance pupil diameter ofthe optical image capturing system; HOS is a distance between anobject-side surface of the first lens and the first image plane on theoptical axis; HOI is a maximum image height on the first image planeperpendicular to the optical axis; InTL is a distance on the opticalaxis from the object-side surface of the first lens to the image-sidesurface of the seventh lens; HAF is a half of a maximum view angle ofthe optical image capturing system; for any surface of any lens; FS is adistance on the optical axis between the first image plane and thesecond image plane.
 2. The optical image capturing system of claim 1,wherein a wavelength of the infrared light ranges from 700 nm to 1300nm, and the first spatial frequency is denoted by SP1, which satisfiesthe following condition: SP1≤440 cycles/mm.
 3. The optical imagecapturing system of claim 1, wherein the optical image capturing systemfurther satisfies:0.9≤2(ARE/HEP)≤2.0; where ARE is a profile curve length measured from astart point where the optical axis of the belonging optical imagecapturing system passes through the surface of the lens, along a surfaceprofile of the lens, and finally to a coordinate point of aperpendicular distance where is a half of the entrance pupil diameteraway from the optical axis.
 4. The optical image capturing system ofclaim 1, wherein at least one lens among the first lens to the seventhlens is made of glass.
 5. The optical image capturing system of claim 1,wherein the optical image capturing system further satisfies:HOS/HOI≥1.2.
 6. The optical image capturing system of claim 1, whereinat least one surface of each of at least one lens among the first lensto the seventh lens has at least an inflection point.
 7. The opticalimage capturing system of claim 1, wherein the optical image capturingsystem further satisfies:0.05≤ARE71/TP7≤35; and0.05≤ARE72/TP7≤35; where ARE71 is a profile curve length measured from astart point where the optical axis passes the object-side surface of theseventh lens, along a surface profile of the object-side surface of theseventh lens, and finally to a coordinate point of a perpendiculardistance where is a half of the entrance pupil diameter away from theoptical axis; ARE72 is a profile curve length measured from a startpoint where the optical axis passes the image-side surface of theseventh lens, along a surface profile of the image-side surface of theseventh lens, and finally to a coordinate point of a perpendiculardistance where is a half of the entrance pupil diameter away from theoptical axis; TP7 is a thickness of the seventh lens on the opticalaxis.
 8. The optical image capturing system of claim 1, wherein theoptical image capturing system further satisfies:PLTA≤100 μm;PSTA≤100 μm;NLTA≤100 μm;NSTA≤100 μm;SLTA≤100 μm;SSTA≤100 μm; and|TDT|<100%; where TDT is a TV distortion; PLTA is a transverseaberration at 0.7 HOI on the image plane in the positive direction of atangential fan of the optical image capturing system after a longestoperation wavelength passing through an edge of the aperture; PSTA is atransverse aberration at 0.7 HOI on the image plane in the positivedirection of the tangential fan after a shortest operation wavelengthpassing through the edge of the aperture; NLTA is a transverseaberration at 0.7 HOI on the image plane in the negative direction ofthe tangential fan after the longest operation wavelength passingthrough the edge of the aperture; NSTA is a transverse aberration at 0.7HOI on the image plane in the negative direction of the tangential fanafter the shortest operation wavelength passing through the edge of theaperture; SLTA is a transverse aberration at 0.7 HOI on the image planeof a sagittal fan of the optical image capturing system after thelongest operation wavelength passing through the edge of the aperture;SSTA is a transverse aberration at 0.7 HOI on the image plane of asagittal fan after the shortest operation wavelength passing through theedge of the aperture.
 9. The optical image capturing system of claim 1,further comprising an aperture, wherein the optical image capturingsystem further satisfies:0.2≤InS/HOS≤1.1; where InS is a distance between the aperture and thefirst image plane on the optical axis.
 10. An optical image capturingsystem, in order along an optical axis from an object side to an imageside, comprising: a first lens having refractive power; a second lenshaving refractive power; a third lens having refractive power; a fourthlens having refractive power; a fifth lens having refractive power; asixth lens having refractive power; a seventh lens having refractivepower; a first image plane, which is an image plane specifically forvisible light and perpendicular to the optical axis; a through-focusmodulation transfer rate (value of MTF) at a first spatial frequencyhaving a maximum value at central field of view of the first imageplane, and the first spatial frequency being 110 cycles/mm; and a secondimage plane, which is an image plane specifically for infrared light andperpendicular to the optical axis; the through-focus modulation transferrate (value of MTF) at the first spatial frequency having a maximumvalue at central of field of view of the second image plane, and thefirst spatial frequency being 110 cycles/mm; wherein the optical imagecapturing system consists of the seven lenses with refractive power; atleast one lens among the first lens to the seventh lens has positiverefractive power; each lens among the first lens to the seventh lens hasan object-side surface, which faces the object side, and an image-sidesurface, which faces the image side; wherein the optical image capturingsystem satisfies:1.0≤f/HEP≤10.0;0 deg<HAF≤150 deg;|FS|≤60 μm; and0.9≤2(ARE/HEP)≤2.0; where f1, f2, f3, f4, f5, f6, and f7 are focallengths of the first lens to the seventh lens, respectively; f is afocal length of the optical image capturing system; HOI is a maximumheight for image formation perpendicular to the optical axis on theimage plane; HEP is an entrance pupil diameter of the optical imagecapturing system; HOS is a distance between the object-side surface ofthe first lens and the first image plane on the optical axis; InTL is adistance on the optical axis from the object-side surface of the firstlens to the image-side surface of the seventh lens; HAF is a half of amaximum view angle of the optical image capturing system; for anysurface of any lens; FS is a distance on the optical axis between thefirst image plane and the second image plane; ARE is a profile curvelength measured from a start point where the optical axis passestherethrough, along a surface profile thereof, and finally to acoordinate point of a perpendicular distance where is a half of theentrance pupil diameter away from the optical axis.
 11. The opticalimage capturing system of claim 10, wherein the optical image capturingsystem further satisfies:0.9≤ARS/EHD≤2.0; where, for any surface of any lens, EHD is a maximumeffective half diameter thereof, ARS is a profile curve length measuredfrom a start point where the optical axis passes therethrough, along asurface profile thereof, and finally to an end point of the maximumeffective half diameter thereof.
 12. The optical image capturing systemof claim 10, wherein each two neighboring lenses among the first to theseventh lenses are separated by air.
 13. The optical image capturingsystem of claim 10, wherein the optical image capturing system furthersatisfies:0<IN45/f≤3.0; where IN45 is a distance on the optical axis between thefourth lens and the fifth lens.
 14. The optical image capturing systemof claim 10, wherein the optical image capturing system furthersatisfies:0<IN56/f≤5; where IN56 is a distance on the optical axis between thefifth lens and the sixth lens.
 15. The optical image capturing system ofclaim 10, wherein the optical image capturing system further satisfies:HOS/HOI≥1.2.
 16. The optical image capturing system of claim 10, whereinat least one lens among the first lens to the seventh lens is a lightfilter, which is capable of filtering out light of wavelengths shorterthan 500 nm.
 17. The optical image capturing system of claim 10, whereinat least one lens among the first lens to the seventh lens are made ofglass.
 18. The optical image capturing system of claim 10, wherein halfof a vertical maximum viewable angle of the optical image capturingsystem is denoted by VHAF, and the following condition is satisfied:VHAF≥20 deg.
 19. The optical image capturing system of claim 10, whereinthe optical image capturing system further satisfies:0.1≤(TP7+IN67)/TP6≤50; where IN67 is a distance on the optical axisbetween the sixth lens and the seventh lens; TP6 is a thickness of thesixth lens on the optical axis; TP7 is a thickness of the seventh lenson the optical axis.
 20. An optical image capturing system, in orderalong an optical axis from an object side to an image side, comprising:a first lens having refractive power; a second lens having refractivepower; a third lens having refractive power; a fourth lens havingrefractive power; a fifth lens having refractive power; a sixth lenshaving refractive power; a seventh lens having refractive power; a firstaverage image plane, which is an image plane specifically for visiblelight and perpendicular to the optical axis; the first average imageplane being installed at the average position of the defocusingpositions, where through-focus modulation transfer rates (values of MTF)of the visible light at central field of view, 0.3 field of view, and0.7 field of view are at their respective maximum at a first spatialfrequency; the first spatial frequency being 110 cycles/mm; and a secondaverage image plane, which is an image plane specifically for infraredlight and perpendicular to the optical axis; the second average imageplane being installed at the average position of the defocusingpositions, where through-focus modulation transfer rates of the infraredlight (values of MTF) at central field of view, 0.3 field of view, and0.7 field of view are at their respective maximum at the first spatialfrequency; the first spatial frequency being 110 cycles/mm; wherein theoptical image capturing system consists of the seven lenses havingrefractive power; at least one lens among the first lens to the seventhlens is made of glass; each lens among the first lens to the seventhlens has an object-side surface, which faces the object side, and animage-side surface, which faces the image side; wherein the opticalimage capturing system satisfies:1≤f/HEP≤10;0 deg<HAF≤150 deg;|AFS|≤60 μm; and0.9≤2(ARE/HEP)≤2.0; where f1, f2, f3, f4, f5, f6, and f7 are focallengths of the first lens to the seventh lens, respectively; f is afocal length of the optical image capturing system; HEP is an entrancepupil diameter of the optical image capturing system; HAF is a half of amaximum view angle of the optical image capturing system; HOS is adistance between an object-side surface of the first lens and the imageplane on the optical axis; HOI is a maximum image height on the firstimage plane perpendicular to the optical axis; InTL is a distance on theoptical axis from the object-side surface of the first lens to theimage-side surface of the seventh lens; AFS is a distance on the opticalaxis between the first average image plane and the second average imageplane; ARE is a profile curve length measured from a start point wherethe optical axis passes therethrough, along a surface profile thereof,and finally to a coordinate point of a perpendicular distance where is ahalf of the entrance pupil diameter away from the optical axis.
 21. Theoptical image capturing system of claim 20, wherein the optical imagecapturing system further satisfies:0.9≤ARS/EHD≤2.0; where, for any surface of any lens, EHD is a maximumeffective half diameter thereof, ARS is a profile curve length measuredfrom a start point where the optical axis passes therethrough, along asurface profile thereof, and finally to an end point of the maximumeffective half diameter thereof.
 22. The optical image capturing systemof claim 20, wherein each two neighboring lenses among the first to theseventh lenses are separated by air.
 23. The optical image capturingsystem of claim 20, wherein the optical image capturing system furthersatisfies:HOS/HOI≥1.6.
 24. The optical image capturing system of claim 20, whereina linear magnification of an image formed by the optical image capturingsystem on the second average image plane is LM, which satisfies thefollowing condition: LM≥0.0003.
 25. The optical image capturing systemof claim 20, further comprising an aperture and an image sensor, whereinthe image sensing device is disposed on the first average image planeand comprises at least 100 thousand pixels; the optical image capturingsystem further satisfies:0.2≤InS/HOS≤1.1; where InS is a distance between the aperture and thefirst average image plane on the optical axis.